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JP7660970B2 - Log likelihood ratio calculation circuit and wireless receiving device - Google Patents
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JP7660970B2 - Log likelihood ratio calculation circuit and wireless receiving device - Google Patents

Log likelihood ratio calculation circuit and wireless receiving device Download PDF

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JP7660970B2
JP7660970B2 JP2020186373A JP2020186373A JP7660970B2 JP 7660970 B2 JP7660970 B2 JP 7660970B2 JP 2020186373 A JP2020186373 A JP 2020186373A JP 2020186373 A JP2020186373 A JP 2020186373A JP 7660970 B2 JP7660970 B2 JP 7660970B2
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賢晃 加藤
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Japan Radio Co Ltd
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この発明は、対数尤度比算出回路および無線受信装置に関し、特に、低密度パリティ検査復号における誤り訂正において使用される対数尤度比を算出する回路および前記回路を含む無線受信装置に関する。 This invention relates to a log-likelihood ratio calculation circuit and a wireless receiving device, and in particular to a circuit that calculates a log-likelihood ratio used in error correction in low-density parity check decoding and a wireless receiving device that includes the circuit.

従来、低密度パリティ検査(LDPC:Low Density Parity Check の略)復号において、受信信号の熱雑音の分布に基づいて算出した対数尤度比(LLR:Log-Likelihood Ratio の略)を使用して誤り訂正を行う手法が知られている(例えば特許文献1参照)。 Conventionally, in low density parity check (LDPC) decoding, a method for performing error correction using a log-likelihood ratio (LLR: Log-Likelihood Ratio) calculated based on the distribution of thermal noise in the received signal is known (see, for example, Patent Document 1).

特開2013-201582号公報JP 2013-201582 A

ところで、高多値の変調方式では、受信信号の位相雑音やフェージングなど熱雑音以外の影響も大きく、低密度パリティ検査の誤り訂正能力が低減する、という問題がある。具体的には、従来の対数尤度比の算出方法では、受信信号の熱雑音によって理想シンボル点を中心として正規分布/ガウス分布に基づいて受信信号の振幅が変動することを前提としている。しかしながら、この方法では、受信信号の位相雑音やフェージングなどによってシンボルの位相が回転した際の変動を考慮することができない。このため、特に位相雑音が存在する環境下において対数尤度比の算出精度が劣化し、延いては低密度パリティ検査の誤り訂正能力が低減してしまう。 However, in high-multiple-level modulation methods, there is a problem in that the error correction capability of the low-density parity check is reduced due to the large influence of factors other than thermal noise, such as phase noise and fading of the received signal. Specifically, the conventional method of calculating the log-likelihood ratio assumes that the amplitude of the received signal fluctuates based on a normal distribution/Gaussian distribution centered on the ideal symbol point due to thermal noise in the received signal. However, this method cannot take into account the fluctuation that occurs when the phase of the symbol rotates due to phase noise and fading of the received signal. For this reason, the calculation accuracy of the log-likelihood ratio deteriorates, especially in an environment where phase noise is present, and ultimately the error correction capability of the low-density parity check is reduced.

そこでこの発明は、対数尤度比の算出精度を向上させて低密度パリティ検査の誤り訂正能力を向上させることが可能な、対数尤度比算出回路および前記対数尤度比算出回路を含む無線受信装置を提供することを目的とする。 The present invention aims to provide a log-likelihood ratio calculation circuit and a wireless receiving device including the log-likelihood ratio calculation circuit that can improve the accuracy of calculating the log-likelihood ratio and thereby improve the error correction capability of the low-density parity check.

上記課題を解決するために、請求項1に記載の発明は、熱雑音に基づく対数尤度比と位相雑音に基づく対数尤度比とのそれぞれに重み係数を乗じたうえで加算して対数尤度比を算出する対数尤度比算出回路であって前記位相雑音に基づく対数尤度比を、送信側において多値数が16の直角位相振幅変調方式で変調された4bitの受信信号のうち、理想シンボル点の位相角度に応じて0になるか1になるかが区別されているbitについては、前記受信信号の位相角度を用いて、位相角度に応じて0になる確率密度分布と1になる確率密度分布とに基づいて算出し、振幅に応じて0になるか1になるかが区別されている理想シンボル点(「振幅区別シンボル点」と呼ぶ)と位相角度に応じて0になるか1になるかが区別されている理想シンボル点(「位相区別シンボル点」と呼ぶ)とに分けられるbitについては、前記振幅区別シンボル点と前記位相区別シンボル点とのうちのどちらであるかを前記受信信号の振幅に基づいて判断したうえで、前記振幅区別シンボル点について、前記受信信号の振幅を用いて、振幅に応じて0になる確率密度分布と1になる確率密度分布とに基づいて算出し、前記位相区別シンボル点について、前記受信信号の位相角度を用いて、位相角度に応じて0になる確率密度分布と1になる確率密度分布とに基づいて算出する、ことを特徴とする対数尤度比算出回路である。 In order to solve the above problem, the invention described in claim 1 is a log likelihood ratio calculation circuit that calculates a log likelihood ratio by multiplying a log likelihood ratio based on thermal noise and a log likelihood ratio based on phase noise by a weighting factor and then adding them up, and calculates the log likelihood ratio based on the phase noise based on a probability density distribution that becomes 0 and a probability density distribution that becomes 1 according to the phase angle of an ideal symbol point that becomes 0 or 1 according to the amplitude of the ideal symbol point ("amplitude discrimination signal") that becomes 0 or 1 according to the amplitude of the ... and an ideal symbol point (called a "phase-distinguishing symbol point") which is distinguished as being 0 or 1 depending on a phase angle, the circuit determines whether the bit is the amplitude-distinguishing symbol point or the phase-distinguishing symbol point based on the amplitude of the received signal, and then calculates the amplitude-distinguishing symbol point based on a probability density distribution which becomes 0 and a probability density distribution which becomes 1 depending on the amplitude using the amplitude of the received signal, and calculates the phase-distinguishing symbol point based on a probability density distribution which becomes 0 and a probability density distribution which becomes 1 depending on the phase angle using the phase angle of the received signal .

請求項に記載の発明は、請求項に記載の対数尤度比算出回路において、所定の数式に従って各bitの位相雑音に基づく対数尤度比を算出する、ことを特徴とする。 According to a second aspect of the present invention, in the log-likelihood ratio calculation circuit according to the first aspect, a log-likelihood ratio based on the phase noise of each bit is calculated according to a predetermined formula.

請求項に記載の発明は、請求項1または2のいずれか1項に記載の対数尤度比算出回路を備える、ことを特徴とする無線受信装置である。 A third aspect of the present invention provides a radio receiving device comprising the log-likelihood ratio calculation circuit according to the first or second aspect of the present invention.

請求項1乃至請求項に記載の発明によれば、熱雑音に基づく対数尤度比と位相雑音に基づく対数尤度比との相互の優先の度合いを考慮したうえで(具体的には、対数尤度比それぞれに重み係数を乗じたうえで)これらを加算して各bitの対数尤度比を算出することにより、対数尤度比の算出に熱雑音の影響に加えて位相雑音やフェージングによる分布変動の要素を考慮するようにしているので、位相雑音を含む外乱に対してロバストな低密度パリティ検査を実現することが可能となる。 According to the invention described in claims 1 and 2 , the log-likelihood ratio based on thermal noise and the log-likelihood ratio based on phase noise are taken into consideration of the degree of mutual priority between them (specifically, after multiplying each log-likelihood ratio by a weighting coefficient), and then these are added to calculate the log-likelihood ratio for each bit.This takes into account not only the influence of thermal noise, but also factors such as phase noise and distribution fluctuations due to fading when calculating the log-likelihood ratio, making it possible to realize a low-density parity check that is robust against disturbances including phase noise.

請求項1乃至請求項に記載の発明によれば、また、受信信号の位相雑音やフェージングなどによってシンボルの位相が正規分布/ガウス分布に基づいて回転・変動した際の確率分布も考慮して対数尤度比を算出するようにしているので、受信信号の位相雑音が支配的な環境下においても対数尤度比の算出精度を向上させることが可能となり、延いては、低密度パリティ検査の誤り訂正能力を向上させることが可能となる。 According to the inventions described in claims 1 and 2 , the log-likelihood ratio is calculated taking into account the probability distribution when the phase of the symbol rotates or fluctuates based on a normal distribution/Gaussian distribution due to phase noise or fading of the received signal, etc., so that it is possible to improve the calculation accuracy of the log-likelihood ratio even in an environment where phase noise of the received signal is dominant, and ultimately to improve the error correction capability of the low-density parity check.

請求項に記載の発明によれば、対数尤度比を使用して低密度パリティ検査復号における誤り訂正を行う無線受信装置において上記の作用効果を奏することが可能となる。

According to the third aspect of the present invention, the above-mentioned advantageous effects can be achieved in a wireless receiving device that performs error correction in low-density parity check decoding using a log-likelihood ratio.

この発明の実施の形態に係る対数尤度比算出回路としてのLLR算出部を含む、実施の形態における無線受信装置の概略構成を示す機能ブロック図である。1 is a functional block diagram showing a schematic configuration of a wireless receiving device according to an embodiment of the present invention, including an LLR calculation unit as a log-likelihood ratio calculation circuit. 実施の形態に係る対数尤度比算出回路としてのLLR算出部の概略構成を示す機能ブロック図である。1 is a functional block diagram showing a schematic configuration of an LLR calculation unit serving as a log-likelihood ratio calculation circuit according to an embodiment; 16QAM方式の理想シンボル点の配置および各理想シンボル点に割り当てられているbit列を示す図である。1 is a diagram showing an arrangement of ideal symbol points in a 16QAM system and bit sequences assigned to each ideal symbol point; 対数尤度比の算出に纏わる変数の設定を説明する図である。FIG. 13 is a diagram for explaining the setting of variables related to the calculation of a log-likelihood ratio. 1bit目の対数尤度比の算出式の考え方を説明する図であり、特に1bit目が0の領域と1bit目が1の領域とを説明する図である。FIG. 13 is a diagram for explaining the concept of a calculation formula for a log-likelihood ratio of the 1st bit, and in particular, a diagram for explaining a region where the 1st bit is 0 and a region where the 1st bit is 1. 1bit目の対数尤度比の算出式の考え方を説明する図である。FIG. 13 is a diagram for explaining the concept of a calculation formula for a log-likelihood ratio of the first bit. 2bit目の対数尤度比の算出式の考え方を説明する図であり、特に振幅にbit情報をのせているシンボルと位相にbit情報をのせているシンボルとを説明する図である。FIG. 13 is a diagram for explaining the concept of a calculation formula for the log-likelihood ratio of the second bit, and in particular, a diagram for explaining a symbol having bit information carried on the amplitude and a symbol having bit information carried on the phase. 2bit目の対数尤度比の算出式の考え方を説明する図である。FIG. 13 is a diagram for explaining the concept of a calculation formula for the log-likelihood ratio of the second bit. 対数尤度比の重み係数の考え方を説明する図である。(A)は熱雑音に基づく対数尤度比が優先される場合を説明する図である。(B)は位相雑音に基づく対数尤度比が優先される場合を説明する図である。1A is a diagram for explaining the concept of a weighting coefficient of a log-likelihood ratio, and FIG. 1B is a diagram for explaining a case where a log-likelihood ratio based on thermal noise is prioritized, and FIG. 1B is a diagram for explaining a case where a log-likelihood ratio based on phase noise is prioritized. 従来の対数尤度比の算出方法の問題点とこの発明に係る対数尤度比算出回路による対策とを説明する図である。1 is a diagram for explaining problems with a conventional method for calculating a log-likelihood ratio and a countermeasure by a log-likelihood ratio calculation circuit according to the present invention; この発明に係る対数尤度比算出回路の有効性の検証例で用いられた評価系の概略構成を示す機能ブロック図である。FIG. 1 is a functional block diagram showing a schematic configuration of an evaluation system used in a verification example of the effectiveness of a log-likelihood ratio calculation circuit according to the present invention. この発明に係る対数尤度比算出回路の有効性の検証例における評価結果としての符号の誤り率を示す図である。13 is a diagram showing a code error rate as an evaluation result in a verification example of the effectiveness of the log-likelihood ratio calculation circuit according to the present invention. FIG.

以下、この発明を図示の実施の形態に基づいて説明する。なお、以下では、この発明の特徴的な構成について説明し、無線通信を行う際の従来と同様の仕組みについては説明を省略する。また、各図では、複素信号を構成する実部(I信号;別言すると、同相成分,I信号成分)を伝送する信号線と虚部(Q信号;別言すると、直交成分,Q信号成分)を伝送する信号線とをまとめて1本の信号線で表示している。また、下記の説明における「以上」と「より大きい」とは相互に置き換えられてもよく、さらに、「以下」と「未満」とは相互に置き換えられてもよい。 The present invention will be described below based on the illustrated embodiment. Note that the following describes the characteristic configuration of the present invention, and the description of the conventional mechanism for wireless communication will be omitted. In addition, in each figure, the signal line transmitting the real part (I signal; in other words, the in-phase component, I signal component) and the signal line transmitting the imaginary part (Q signal; in other words, the quadrature component, Q signal component) of the complex signal are shown together as a single signal line. In addition, in the following description, "greater than or equal to" and "greater than" may be interchangeable, and furthermore, "less than or equal to" and "less than" may be interchangeable.

図1は、この発明の実施の形態に係る対数尤度比算出回路としてのLLR算出部20を含む、実施の形態における無線受信装置1の概略構成を示す機能ブロック図である。 Figure 1 is a functional block diagram showing a schematic configuration of a wireless receiving device 1 according to an embodiment of the present invention, including an LLR calculation unit 20 as a log-likelihood ratio calculation circuit.

アンテナ10は、図示していない無線送信装置から送出された信号波を受信して、前記信号波を受信信号としてチャネルフィルタ11へと転送する。 The antenna 10 receives a signal wave sent from a wireless transmitting device (not shown) and transfers the signal wave to the channel filter 11 as a received signal.

ここで、無線送信装置は、送信対象の無線フレームを、低密度パリティ検査符号化を施すとともに多値数が16の直角位相振幅変調方式(即ち、16QAM方式;QAMは Quadrature Amplitude Modulation の略)で変調したうえでアンテナから送出する。つまり、無線受信装置1は、低密度パリティ検査符号化が施されて多値数が16の直角位相振幅変調方式(16QAM方式)で変調された多値変調信号を受信する。 The wireless transmitting device performs low-density parity check coding on the wireless frame to be transmitted and modulates it using a quadrature amplitude modulation method with a multi-level of 16 (i.e., 16QAM method; QAM is an abbreviation for Quadrature Amplitude Modulation), and then transmits it from the antenna. In other words, the wireless receiving device 1 receives a multi-level modulated signal that has been subjected to low-density parity check coding and modulated using a quadrature amplitude modulation method with a multi-level of 16 (16QAM method).

チャネルフィルタ11は、受信帯域を制限するためのフィルタであり、具体的には例えばバンドパスフィルタによって構成され得る。チャネルフィルタ11は、アンテナ10から転送される受信信号の入力を受け、前記受信信号に対して帯域制限処理を施して、前記受信信号から所望の周波数帯域の受信信号を抽出して出力する。 The channel filter 11 is a filter for limiting the reception band, and specifically may be configured, for example, by a bandpass filter. The channel filter 11 receives the reception signal transferred from the antenna 10, performs band limiting processing on the reception signal, and extracts and outputs the reception signal of the desired frequency band from the reception signal.

ミキサ13は、チャネルフィルタ11から出力される受信信号の入力を受けるとともに局部発振器12から出力されるローカル信号の入力を受け、前記受信信号に前記ローカル信号を乗算して、前記受信信号の周波数を変換(具体的には、ダウンコンバート)して出力する。 The mixer 13 receives the received signal output from the channel filter 11 and the local signal output from the local oscillator 12, multiplies the received signal by the local signal, and converts (specifically, down-converts) the frequency of the received signal and outputs it.

自動利得制御部14は、ミキサ13から出力される受信信号の入力を受け、前記受信信号に対して前記受信信号のレベルが所定のレベルで一定になるように利得調整処理を施して、利得調整処理後(言い換えると、レベル補正後)の受信信号(尚、アナログ信号である)を出力する。 The automatic gain control unit 14 receives the received signal output from the mixer 13, performs gain adjustment processing on the received signal so that the level of the received signal is constant at a predetermined level, and outputs the received signal (which is an analog signal) after gain adjustment processing (in other words, after level correction).

A/D変換器15(Analog-to-Digital converter)は、自動利得制御部14から出力される受信信号の入力を受け、前記受信信号に対してアナログ-デジタル変換処理を施して、アナログ信号からデジタル信号への変換を行う。すなわち、A/D変換器15は、デジタルの受信信号を出力する。 The A/D converter 15 (Analog-to-Digital converter) receives the received signal output from the automatic gain control unit 14, and performs analog-to-digital conversion processing on the received signal to convert it from an analog signal to a digital signal. In other words, the A/D converter 15 outputs a digital received signal.

デジタル直交検波部16は、A/D変換器15から出力されるデジタルの受信信号の入力を受け、前記受信信号を直交検波によってベースバンド信号に変換する。デジタル直交検波部16は、具体的には、数値制御発振器からcos波が入力されて前記受信信号の同相成分を同期検出する乗算器と、数値制御発振器からsin波が入力されて前記受信信号の直交成分を同期検出する乗算器とを備える。デジタル直交検波部16は、デジタル信号処理による多値変調の直交検波を行い、実部を構成する実数成分(I信号)と虚部を構成する虚数成分(Q信号)とのIQ直交座標で表現される複素信号(別言すると、同相成分および直交成分の検波信号)を生成して出力する。 The digital quadrature detection unit 16 receives the digital received signal output from the A/D converter 15 and converts the received signal into a baseband signal by quadrature detection. Specifically, the digital quadrature detection unit 16 includes a multiplier that receives a cosine wave from a numerically controlled oscillator and synchronously detects the in-phase component of the received signal, and a multiplier that receives a sine wave from the numerically controlled oscillator and synchronously detects the quadrature component of the received signal. The digital quadrature detection unit 16 performs quadrature detection of multi-level modulation by digital signal processing, and generates and outputs a complex signal (in other words, a detection signal of the in-phase component and the quadrature component) expressed in IQ quadrature coordinates with the real component (I signal) constituting the real part and the imaginary component (Q signal) constituting the imaginary part.

デジタル直交検波部16の数値制御発振器は、設定値に応じた周波数で発振する発振器であり、位相が90°だけ相互に異なるcos波とsin波とを発生させて2つの乗算器のそれぞれへと供給する。 The numerically controlled oscillator of the digital quadrature detection unit 16 is an oscillator that oscillates at a frequency according to a set value, and generates a cosine wave and a sine wave whose phases differ by 90° from each other, and supplies them to each of the two multipliers.

ロールオフフィルタ17は、デジタル直交検波部16から出力されるベースバンド信号(別言すると、同相成分および直交成分の検波信号)の入力を受け、前記ベースバンド信号の同相成分と直交成分とのそれぞれに対して符号間干渉を除去するための処理を施して、前記ベースバンド信号のスペクトラム波形を所望のロールオフとなるように整形して出力する。 The roll-off filter 17 receives the baseband signal (in other words, the detection signal of the in-phase component and the quadrature component) output from the digital quadrature detection unit 16, processes the in-phase component and the quadrature component of the baseband signal to remove inter-symbol interference, and shapes the spectrum waveform of the baseband signal to have the desired roll-off before outputting it.

等化器18は、ロールオフフィルタ17から出力されるベースバンド信号の入力を受け、前記ベースバンド信号の同相成分と直交成分とのそれぞれに対して、周波数選択性フェージングによる符号間干渉を除去するための適応等化処理を施して、適応等化処理後のベースバンド信号(受信信号)を出力する。 The equalizer 18 receives the baseband signal output from the roll-off filter 17, performs adaptive equalization processing on each of the in-phase and quadrature components of the baseband signal to remove inter-symbol interference caused by frequency selective fading, and outputs the baseband signal after adaptive equalization processing (received signal).

復号部19は、LLR算出部20から出力される対数尤度比(LLR:Log-Likelihood Ratio の略)の入力を受け、前記対数尤度比を使用して例えばsum-product復号法に従って低密度パリティ検査復号処理を行う。 The decoding unit 19 receives the log-likelihood ratio (LLR: abbreviation for Log-Likelihood Ratio) output from the LLR calculation unit 20, and performs low-density parity check decoding processing using the log-likelihood ratio, for example, according to the sum-product decoding method.

LLR算出部20は、低密度パリティ検査復号における誤り訂正において使用される対数尤度比を算出する回路であり、無線受信装置1に組み込まれる。 The LLR calculation unit 20 is a circuit that calculates the log-likelihood ratio used in error correction in low-density parity check decoding, and is incorporated into the wireless receiving device 1.

図2は、実施の形態に係る対数尤度比算出回路としてのLLR算出部20の概略構成を示す機能ブロック図である。 Figure 2 is a functional block diagram showing the schematic configuration of the LLR calculation unit 20 as a log-likelihood ratio calculation circuit according to the embodiment.

実施の形態に係るLLR算出部20は、熱雑音に基づく対数尤度比LLRN(bit_num)と位相雑音に基づく対数尤度比LLRφ(bit_num)とのそれぞれに重み係数WN,Wφを乗じたうえで加算して対数尤度比LLRbit_numを算出する、ようにしている。 The LLR calculation unit 20 according to the embodiment multiplies the log-likelihood ratio LLR N(bit_num) based on thermal noise and the log-likelihood ratio LLRφ (bit_num) based on phase noise by weighting coefficients W N and Wφ, respectively, and then adds them together to calculate the log-likelihood ratio LLR bit_num .

実施の形態に係るLLR算出部20は、さらに、位相雑音に基づく対数尤度比LLRφ(bit_num)を送信側において多値数が16の直角位相振幅変調方式で変調された4bitの受信信号のうち、理想シンボル点の位相角度φiに応じて0になるか1になるかが区別されているbitについては、受信信号の位相角度xφを用いて、位相角度に応じて0になる確率密度分布と1になる確率密度分布とに基づいて算出し、振幅に応じて0になるか1になるかが区別されている理想シンボル点(「振幅区別シンボル点」と呼ぶ)と位相角度に応じて0になるか1になるかが区別されている理想シンボル点(「位相区別シンボル点」と呼ぶ)とに分けられるbitについては、振幅区別シンボル点と位相区別シンボル点とのうちのどちらであるかを受信信号の振幅xRに基づいて判断したうえで、振幅区別シンボル点について、受信信号の振幅xRを用いて、振幅に応じて0になる確率密度分布と1になる確率密度分布とに基づいて算出し、位相区別シンボル点について、受信信号の位相角度xφを用いて、位相角度に応じて0になる確率密度分布と1になる確率密度分布とに基づいて算出する、ようにしている。 The LLR calculation unit 20 according to the embodiment further calculates a log likelihood ratio LLRφ (bit_num) based on phase noise, for bits that are distinguished as being 0 or 1 depending on the phase angle φ i of an ideal symbol point, of a 4-bit received signal modulated by a quadrature phase amplitude modulation method with a multi-level number of 16 on the transmitting side, based on a probability density distribution that becomes 0 and a probability density distribution that becomes 1 depending on the phase angle, using the phase angle xφ of the received signal, and for bits that are classified into an ideal symbol point that is distinguished as being 0 or 1 depending on the amplitude (referred to as an "amplitude-distinguishing symbol point") and an ideal symbol point that is distinguished as being 0 or 1 depending on the phase angle (referred to as a "phase-distinguishing symbol point"), it determines whether the bit is an amplitude-distinguishing symbol point or a phase-distinguishing symbol point based on the amplitude x R of the received signal, and then calculates the log likelihood ratio LLRφ(bit_num) based on the phase noise, using the phase angle xφ of the received signal. Using R , calculations are made based on a probability density distribution which becomes 0 and a probability density distribution which becomes 1 depending on the amplitude, and for the phase-distinguishing symbol points, using the phase angle xφ of the received signal, calculations are made based on a probability density distribution which becomes 0 and a probability density distribution which becomes 1 depending on the phase angle.

まず、16QAM方式の理想シンボル点の配置および各理想シンボル点に割り当てられているbit列(言い換えると、16QAMの信号空間ダイヤグラム)を図3に示す。なお、図3において、Aiは理想シンボル点配置の同相成分であり、Biは理想シンボル点配置の直交成分である(但し、i=1,2,3,4)。 First, the arrangement of ideal symbol points in the 16QAM system and the bit strings assigned to each ideal symbol point (in other words, the signal space diagram of 16QAM) are shown in Fig. 3. In Fig. 3, A i is the in-phase component of the ideal symbol point arrangement, and B i is the quadrature component of the ideal symbol point arrangement (where i = 1, 2, 3, 4).

LLR算出部20は、下記の数式1に従って、(bit_num)bit目の対数尤度比LLRbit_numを算出する。
(数1) LLRbit_num = WN×LLRN(bit_num)+Wφ×LLRφ(bit_num)
ここに、bit_num:ビット番号(但し、bit_num=1,2,3,4)
LLRN(bit_num):熱雑音に基づく対数尤度比
LLRφ(bit_num):位相雑音に基づく対数尤度比
N:熱雑音に基づく対数尤度比の重み係数
Wφ:位相雑音に基づく対数尤度比の重み係数
The LLR calculation unit 20 calculates the log-likelihood ratio LLR bit_num of the (bit_num)th bit according to the following equation 1.
(Math. 1) LLR bit_num = W N ×LLR N(bit_num) +Wφ×LLRφ (bit_num)
Here, bit_num: bit number (where bit_num = 1, 2, 3, 4)
LLR N(bit_num) : Log-likelihood ratio based on thermal noise
LLRφ (bit_num) : Log-likelihood ratio based on phase noise
W N : Weighting factor of log-likelihood ratio based on thermal noise
Wφ: weighting factor of log-likelihood ratio based on phase noise

(bit_num)bit目の熱雑音に基づく対数尤度比LLRN(bit_num)は、具体的には例えば下記の数式2A乃至数式2Dに従って算出される。

Figure 0007660970000001
Specifically, the log-likelihood ratio LLR N(bit_num) based on thermal noise of the (bit_num)th bit is calculated according to, for example, the following Equations 2A to 2D.
Figure 0007660970000001

上記の数式2A乃至数式2Dにおける各記号・変数の意味は下記のとおりである。
LLRN1:1bit目の熱雑音に基づく対数尤度比
LLRN2:2bit目の熱雑音に基づく対数尤度比
LLRN3:3bit目の熱雑音に基づく対数尤度比
LLRN4:4bit目の熱雑音に基づく対数尤度比
i:受信信号の同相成分
q:受信信号の直交成分
i:理想シンボル点配置の同相成分(但し、i=1,2,3,4)
i:理想シンボル点配置の直交成分(但し、i=1,2,3,4)
σ2:雑音分散
The meanings of the symbols and variables in the above formulas 2A to 2D are as follows.
LLR N1 : Log likelihood ratio based on thermal noise of the 1st bit LLR N2 : Log likelihood ratio based on thermal noise of the 2nd bit LLR N3 : Log likelihood ratio based on thermal noise of the 3rd bit LLR N4 : Log likelihood ratio based on thermal noise of the 4th bit x i : In-phase component of the received signal x q : Quadrature component of the received signal A i : In-phase component of the ideal symbol point constellation (where i = 1, 2, 3, 4)
B i : Orthogonal components of the ideal symbol point constellation (where i=1, 2, 3, 4)
σ 2 : Noise variance

(bit_num)bit目の位相雑音に基づく対数尤度比LLRφ(bit_num)は、具体的には例えば下記の数式3乃至数式6に従って算出される。ここで、図3に示す理想シンボル点の配置に対して規定される、下記の数式3乃至数式6で用いられる変数の設定を図4に示す。 Specifically, the log-likelihood ratio LLRφ (bit_num) based on the phase noise of the (bit_num)th bit is calculated, for example, according to the following formulas 3 to 6. Here, the settings of variables used in the following formulas 3 to 6, which are defined for the arrangement of ideal symbol points shown in FIG. 3, are shown in FIG.

下記の数式3乃至数式7における各記号・変数の意味は下記のとおりである。なお、下記のうちの理想シンボル点の位相角度の「φ」は、図面では「Φ」として表示している。
xφ:受信信号の位相角度
R:受信信号の振幅
φi:理想シンボル点の位相角度(但し、φの添字i=0,1,2,・・・,11)
i:理想シンボル点の振幅(但し、Rの添字i=0,1,2)
σ2:雑音分散
thre1:第1の振幅閾値
thre2:第2の振幅閾値
The meanings of the symbols and variables in the following Equations 3 to 7 are as follows: Note that the phase angle "φ" of the ideal symbol point in the following equations is represented as "Φ" in the drawings.
xφ: Phase angle of the received signal x R : Amplitude of the received signal φ i : Phase angle of the ideal symbol point (where the subscript i of φ is 0, 1, 2, ..., 11)
R i : Amplitude of the ideal symbol point (where the subscript i of R = 0, 1, 2)
σ 2 : Noise variance R thre1 : First amplitude threshold R thre2 : Second amplitude threshold

1bit目の位相雑音に基づく対数尤度比LLRφ1は、下記の数式3に従って算出される。

Figure 0007660970000002
The log-likelihood ratio LLRφ 1 based on the phase noise of the first bit is calculated according to the following Equation 3.
Figure 0007660970000002

2bit目の位相雑音に基づく対数尤度比LLRφ2は、受信信号の振幅xRが第1の振幅閾値Rthre1以上または第2の振幅閾値Rthre2以下(即ち、xR≧Rthre1 または xR≦Rthre2)の場合に下記の数式4Aに従って算出され、受信信号の振幅xRが第1の振幅閾値Rthre1未満かつ第2の振幅閾値Rthre2より大きい(即ち、Rthre2<xR<Rthre1)の場合に下記の数式4Bに従って算出される。

Figure 0007660970000003
The log-likelihood ratio LLRφ2 based on the phase noise of the second bit is calculated according to the following formula 4A when the amplitude xR of the received signal is equal to or greater than the first amplitude threshold Rthre1 or equal to or less than the second amplitude threshold Rthre2 (i.e., xRRthre1 or xRRthre2 ), and is calculated according to the following formula 4B when the amplitude xR of the received signal is less than the first amplitude threshold Rthre1 and greater than the second amplitude threshold Rthre2 (i.e., Rthre2 < xR < Rthre1 ).
Figure 0007660970000003

3bit目の位相雑音に基づく対数尤度比LLRφ3は、下記の数式5に従って算出される。

Figure 0007660970000004
The log-likelihood ratio LLRφ 3 based on the phase noise of the third bit is calculated according to the following Equation 5.
Figure 0007660970000004

4bit目の位相雑音に基づく対数尤度比LLRφ4は、受信信号の振幅xRが第1の振幅閾値Rthre1以上または第2の振幅閾値Rthre2以下(即ち、xR≧Rthre1 または xR≦Rthre2)の場合に下記の数式6Aに従って算出され、受信信号の振幅xRが第1の振幅閾値Rthre1未満かつ第2の振幅閾値Rthre2より大きい(即ち、Rthre2<xR<Rthre1)の場合に下記の数式6Bに従って算出される。

Figure 0007660970000005
The log-likelihood ratio LLRφ4 based on the phase noise of the 4th bit is calculated according to the following formula 6A when the amplitude xR of the received signal is equal to or greater than the first amplitude threshold Rthre1 or equal to or less than the second amplitude threshold Rthre2 (i.e., xRRthre1 or xRRthre2 ), and is calculated according to the following formula 6B when the amplitude xR of the received signal is less than the first amplitude threshold Rthre1 and greater than the second amplitude threshold Rthre2 (i.e., Rthre2 < xR < Rthre1 ).
Figure 0007660970000005

上記の数式3乃至数式6は下記の考え方に基づいている(図5乃至図8参照)。 The above formulas 3 to 6 are based on the following idea (see Figures 5 to 8).

1bit目は、位相角度が-90°から+90°(言い換えると、270°から360°/0°を経て90°;即ち、図5において理想シンボル点の位相角度Φ9からΦ11,Φ0を経てΦ2までを含むIQ直交座標系の第4象限および第1象限)のときに0になり、位相角度が+90°から-90°(言い換えると、90°から180°を経て270°;即ち、図5において理想シンボル点の位相角度Φ3からΦ5,Φ6を経てΦ8までを含むIQ直交座標系の第2象限および第3象限)のときに1になる。したがって、受信信号の位相が正規分布/ガウス分布に基づいて揺らぐと考えた場合、1bit目が0になる確率密度は図6Aのように示され、1bit目が1になる確率密度は図6Bのように示される。これに基づいて、これら確率密度分布を各項として考慮することにより、1bit目の位相雑音に基づく対数尤度比LLRφ1を算出する上記の数式3が導出される(図6C参照)。 The first bit is 0 when the phase angle is -90° to +90° (in other words, 270° to 90° through 360°/0°; that is, the fourth and first quadrants of the IQ orthogonal coordinate system including the phase angles of the ideal symbol points Φ 9 to Φ 11 , Φ 0 to Φ 2 in FIG. 5 ), and is 1 when the phase angle is +90° to -90° (in other words, 270° through 180°; that is, the second and third quadrants of the IQ orthogonal coordinate system including the phase angles of the ideal symbol points Φ 3 to Φ 5 , Φ 6 to Φ 8 in FIG. 5 ). Therefore, if it is considered that the phase of the received signal fluctuates based on a normal distribution/Gaussian distribution, the probability density of the first bit being 0 is shown as in FIG. 6A, and the probability density of the first bit being 1 is shown as in FIG. 6B. Based on this, by considering these probability density distributions as each term, the above-mentioned formula 3 for calculating the log-likelihood ratio LLRφ 1 based on the phase noise of the 1st bit is derived (see FIG. 6C).

3bit目も1bit目と同様の考え方に基づいており、すなわち、3bit目は、位相角度が0°から+90°を経て+180°(即ち、図5において理想シンボル点の位相角度Φ0からΦ2,Φ3を経てΦ5までを含むIQ直交座標系の第1象限および第2象限)のときに0になり、位相角度が+180°から+270°を経て0°(即ち、図5において理想シンボル点の位相角度Φ6からΦ8,Φ9を経てΦ11までを含むIQ直交座標系の第3象限および第4象限)のときに1になる。これに基づいて、3bit目が0になる確率密度分布と3bit目が1になる確率密度分布とを各項として考慮することにより、3bit目の位相雑音に基づく対数尤度比LLRφ3を算出する上記の数式5が導出される。 The third bit is based on the same idea as the first bit, that is, the third bit becomes 0 when the phase angle goes from 0° through +90° to +180° (i.e., the first and second quadrants of the IQ orthogonal coordinate system including the phase angles of the ideal symbol points Φ 0 through Φ 2 , Φ 3 to Φ 5 in FIG. 5 ), and becomes 1 when the phase angle goes from +180° through +270° to 0° (i.e., the third and fourth quadrants of the IQ orthogonal coordinate system including the phase angles of the ideal symbol points Φ 6 through Φ 8 , Φ 9 to Φ 11 in FIG. 5 ). Based on this, the above-mentioned Equation 5 for calculating the log-likelihood ratio LLRφ 3 based on the phase noise of the third bit is derived by considering the probability density distribution in which the third bit is 0 and the probability density distribution in which the third bit is 1 as each term.

また、2bit目については、IQ直交座標系のすべての象限で同じ考え方ができるため、IQ直交座標系の第1象限を例に挙げて説明する。2bit目は、図7に示すように、0となるか1となるかが振幅によって区別されている理想シンボル点(同図中の「振幅にbit情報をのせているシンボル」;尚、振幅区別シンボル点である)と、0となるか1となるかが位相によって区別されている理想シンボル点(同図中の「位相にbit情報をのせているシンボル」;尚、位相区別シンボル点である)とに分かれる。このため、受信信号の振幅xRを第1の振幅閾値Rthre1および第2の振幅閾値Rthre2と比較することにより、受信した信号/シンボルがbit情報を振幅と位相とのうちのどちらにのせているかを判断して、それぞれで対数尤度比の算出方法を変えるようにしている。振幅にbit情報をのせているシンボルについて2bit目が0になる確率密度分布と2bit目が1になる確率密度分布とはそれぞれ図8Aのように示され、位相にbit情報をのせているシンボルについて2bit目が0になる確率密度分布と2bit目が1になる確率密度分布とはそれぞれ図8Bのように示される。これに基づいて、これら確率密度分布を各項として考慮することにより、2bit目の位相雑音に基づく対数尤度比LLRφ2を算出する上記の数式4が導出される(図8C参照)。 As for the second bit, the same concept can be applied to all quadrants of the IQ orthogonal coordinate system, so the first quadrant of the IQ orthogonal coordinate system will be taken as an example for explanation. As shown in FIG. 7, the second bit is divided into an ideal symbol point where the amplitude determines whether it is 0 or 1 (the "symbol with bit information on the amplitude" in the figure; this is an amplitude-distinguishing symbol point), and an ideal symbol point where the phase determines whether it is 0 or 1 (the "symbol with bit information on the phase" in the figure; this is a phase-distinguishing symbol point). For this reason, the amplitude xR of the received signal is compared with the first amplitude threshold Rthre1 and the second amplitude threshold Rthre2 to determine whether the received signal/symbol has bit information on the amplitude or phase, and the method of calculating the log-likelihood ratio is changed for each. For a symbol carrying bit information in the amplitude, the probability density distribution in which the second bit is 0 and the probability density distribution in which the second bit is 1 are shown in Fig. 8A, and for a symbol carrying bit information in the phase, the probability density distribution in which the second bit is 0 and the probability density distribution in which the second bit is 1 are shown in Fig. 8B. Based on this, by considering these probability density distributions as each term, the above-mentioned formula 4 for calculating the log-likelihood ratio LLRφ2 based on the phase noise of the second bit is derived (see Fig. 8C).

4bit目も2bit目と同様の考え方に基づいており、振幅にbit情報をのせているシンボルについては2bit目と同様に、また、位相にbit情報をのせているシンボルについては、4bit目が0になるのは理想シンボル点の位相角度がΦ2,Φ3,Φ8,およびΦ9であるとともに1になるのは理想シンボル点の位相角度がΦ0,Φ5,Φ6,およびΦ11であることを踏まえて、振幅にbit情報をのせているシンボルについて4bit目が0になる確率密度分布と4bit目が1になる確率密度分布ならびに位相にbit情報をのせているシンボルについて4bit目が0になる確率密度分布と4bit目が1になる確率密度分布とを各項として考慮することにより、4bit目の位相雑音に基づく対数尤度比LLRφ4を算出する上記の数式6が導出される。 The fourth bit is based on the same idea as the second bit, and in the same way as the second bit, for symbols which carry bit information in amplitude, and for symbols which carry bit information in phase, the fourth bit is 0 at phase angles of the ideal symbol point Φ2 , Φ3 , Φ8 , and Φ9 and 1 at phase angles of the ideal symbol point Φ0 , Φ5 , Φ6 , and Φ11. By considering the probability density distribution where the fourth bit is 0 and the probability density distribution where the fourth bit is 1 for symbols which carry bit information in amplitude, and the probability density distribution where the fourth bit is 0 and the probability density distribution where the fourth bit is 1 for symbols which carry bit information in phase, as each term, the above formula 6 for calculating the log-likelihood ratio LLRφ4 based on the phase noise of the fourth bit can be derived.

第1の振幅閾値Rthre1や第2の振幅閾値Rthre2は、特定の値に限定されるものではなく、例えば第1の振幅閾値Rthre1は理想シンボル点の振幅R1とR2との間に設定されるとともに第2の振幅閾値Rthre2は理想シンボル点の振幅R0とR1との間に設定されたうえで振幅にbit情報をのせているシンボルと位相にbit情報をのせているシンボルとを良好に判別し得ることが考慮されるなどしたうえで適当な値に適宜設定される。具体的には例えば、第1の振幅閾値Rthre1は下記の数式7Aのように設定され、第2の振幅閾値Rthre2は下記の数式7Bのように設定されることが考えられる。
(数7A) Rthre1 = R1+(R2-R1)/2
(数7B) Rthre2 = Ro+(R1-R0)/2
The first amplitude threshold Rthre1 and the second amplitude threshold Rthre2 are not limited to specific values, and for example, the first amplitude threshold Rthre1 is set between the amplitudes R1 and R2 of the ideal symbol points, and the second amplitude threshold Rthre2 is set between the amplitudes R0 and R1 of the ideal symbol points, and are appropriately set to appropriate values while taking into consideration that a symbol having bit information in its amplitude and a symbol having bit information in its phase can be well distinguished. Specifically, for example, the first amplitude threshold Rthre1 may be set as shown in the following formula 7A, and the second amplitude threshold Rthre2 may be set as shown in the following formula 7B.
(Math. 7A) R thre1 = R 1 + (R 2 - R 1 )/2
(Math. 7B) R thre2 = R o +(R 1 - R 0 )/2

そして、上記の数式1に従って算出される対数尤度比を使用して低密度パリティ検査復号処理を行うことにより、熱雑音の分布に基づく対数尤度比LLRNに、位相雑音の分布に基づく対数尤度比LLRφが加えられるので、位相雑音へのロバスト性が向上する。また、位相雑音は熱雑音の大きさやシンボルの位置によって影響の大きさが異なるので、各対数尤度比の重み係数WN,Wφにより、熱雑音と位相雑音とのうちのどちらに基づく対数尤度比を優先するかが制御される。 Then, by performing low-density parity check decoding processing using the log-likelihood ratios calculated according to the above-mentioned formula 1, the log-likelihood ratios LLRφ based on the distribution of phase noise are added to the log-likelihood ratios LLR N based on the distribution of thermal noise, thereby improving robustness against phase noise. Also, since the influence of phase noise differs depending on the magnitude of thermal noise and the position of the symbol, the weighting coefficients W N and Wφ of each log-likelihood ratio control whether the log-likelihood ratio based on thermal noise or phase noise is to be prioritized.

各対数尤度比の重み係数WN,Wφは、それぞれ、特定の値に限定されるものではなく、位相雑音は熱雑音の大きさやシンボルの位置によって影響の大きさが異なることを踏まえて熱雑音と位相雑音とのうちのどちらに基づく対数尤度比をどの程度優先するかが考慮されるなどしたうえで適当な値に適宜設定される。 The weighting coefficients WN , Wφ of each log-likelihood ratio are not limited to specific values, but are appropriately set to appropriate values after taking into consideration the degree to which the log-likelihood ratio based on thermal noise or phase noise is to be prioritized, taking into account that the influence of phase noise varies depending on the magnitude of thermal noise and the position of the symbol.

各対数尤度比の重み係数WN,Wφは、各々所定の算出式によって算出されるようにしてもよく、具体的には例えば下記の数式8Aに従って熱雑音に基づく対数尤度比の重み係数WNが算出されるとともに下記の数式8Bに従って位相雑音に基づく対数尤度比の重み係数WNが算出されるようにしてもよい。

Figure 0007660970000006
The weighting coefficients W N , Wφ of each log-likelihood ratio may be calculated by a predetermined calculation formula. Specifically, for example, the weighting coefficient W N of the log-likelihood ratio based on thermal noise may be calculated according to the following formula 8A, and the weighting coefficient W N of the log-likelihood ratio based on phase noise may be calculated according to the following formula 8B.
Figure 0007660970000006

上記の数式8A,8Bにおける各記号・変数の意味は下記のとおりである。
N:熱雑音の分散(即ち、√Nは熱雑音の平均振幅に相当する)
d:QAM方式のシンボル間間隔
α:優先調整係数
β:同等調整係数
The meanings of the symbols and variables in the above formulas 8A and 8B are as follows:
N: Variance of the thermal noise (i.e., √N corresponds to the average amplitude of the thermal noise)
S d : Symbol interval in QAM system α: Priority adjustment coefficient β: Equivalent adjustment coefficient

優先調整係数αは、熱雑音による振幅変動の平均値(即ち、√N)がQAM方式のシンボル間隔Sdの何%以下のときに位相雑音に基づく対数尤度比LLRφを優先するかを決定づけるための係数である。 The priority adjustment coefficient α is a coefficient for determining the percentage or less of the symbol interval Sd of the QAM system at which the log-likelihood ratio LLRφ based on phase noise is prioritized when the average value of the amplitude fluctuation due to thermal noise (i.e., √N ) is less than or equal to that percentage.

優先調整係数αは、特定の値に限定されるものではなく、熱雑音と位相雑音との相互の優先の度合いが考慮されるなどしたうえで、適当な値に適宜設定される。優先調整係数αは、具体的には例えば、あくまで一例として挙げると、0.1~0.5程度の範囲のうちのいずれかの値に設定されることが考えられる。 The priority adjustment coefficient α is not limited to a specific value, but is set to an appropriate value after taking into consideration the degree of priority between thermal noise and phase noise. Specifically, the priority adjustment coefficient α may be set to a value in the range of about 0.1 to 0.5, for example, as one example only.

同等調整係数βは、熱雑音による対数尤度比と位相雑音による対数尤度比との優先度が同等であるときに各対数尤度比の大きさを等しくするための係数である。 The equality adjustment coefficient β is a coefficient for equalizing the magnitude of each log-likelihood ratio when the log-likelihood ratio due to thermal noise and the log-likelihood ratio due to phase noise have equal priority.

同等調整係数βは、特定の値に限定されるものではなく、優先調整係数αの値を前提として、熱雑音による対数尤度比と位相雑音による対数尤度比との優先度が同等であるときに各対数尤度比の大きさを等しくするような値に適宜設定される。 The equality adjustment coefficient β is not limited to a specific value, but is appropriately set to a value that equalizes the magnitude of each log-likelihood ratio when the log-likelihood ratio due to thermal noise and the log-likelihood ratio due to phase noise have equal priority, assuming the value of the priority adjustment coefficient α.

優先調整係数αおよび同等調整係数βは、LLR算出部20の重み係数制御部24に対して予め設定される。 The priority adjustment coefficient α and the equal adjustment coefficient β are set in advance in the weighting coefficient control unit 24 of the LLR calculation unit 20.

各対数尤度比の重み係数WN,Wφが上記の数式8Aおよび数式8Bに従って算出されるようにすることにより、図9Aに示すように、熱雑音の平均振幅√NがQAM方式のシンボル間間隔Sdのα×100[%]よりも大きい場合に、熱雑音に基づく対数尤度比に対する重み係数WNが大きくなり(具体的には、1より大きくなり)、逆に、位相雑音に基づく対数尤度比に対する重み係数Wφは小さくなり(具体的には、1より小さくなり)、つまり熱雑音に基づく対数尤度比が優先されて最終的な対数尤度比LLRbit_numが算出されることになる。なお、図9では、あくまでも一例として、α=0.5に設定されている。 By calculating the weighting coefficients WN and Wφ of each log-likelihood ratio according to the above formula 8A and formula 8B, as shown in Fig. 9A, when the average amplitude √N of thermal noise is larger than α×100[%] of the symbol interval Sd of the QAM method, the weighting coefficient WN for the log-likelihood ratio based on thermal noise becomes large (specifically, becomes larger than 1), and conversely, the weighting coefficient Wφ for the log-likelihood ratio based on phase noise becomes small (specifically, becomes smaller than 1), that is, the log-likelihood ratio based on thermal noise is prioritized to calculate the final log-likelihood ratio LLR bit_num . Note that in Fig. 9, α is set to 0.5 as an example only.

一方、図9Bに示すように、熱雑音の平均振幅√NがQAM方式のシンボル間間隔Sdのα×100[%]以下の場合に、位相雑音に基づく対数尤度比に対する重み係数Wφが大きくなり(具体的には、1以上になり)、逆に、熱雑音に基づく対数尤度比に対する重み係数WNは小さくなり(具体的には、1以下になり)、つまり位相雑音に基づく対数尤度比が優先されて最終的な対数尤度比LLRbit_numが算出されることになる。 On the other hand, as shown in FIG. 9B , when the average amplitude √N of the thermal noise is equal to or less than α×100 [%] of the inter-symbol interval Sd of the QAM system, the weighting factor Wφ for the log-likelihood ratio based on the phase noise becomes large (specifically, becomes 1 or more), and conversely, the weighting factor WN for the log-likelihood ratio based on the thermal noise becomes small (specifically, becomes 1 or less), that is, the log-likelihood ratio based on the phase noise is prioritized in calculating the final log-likelihood ratio LLR bit_num .

なお、数式8は熱雑音の大きさに基づいて(言い換えると、熱雑音を変数として)熱雑音に基づく対数尤度比に対する重み係数WNおよび位相雑音に基づく対数尤度比に対する重み係数Wφが算出されるようにしているが、位相雑音の大きさに基づいて(言い換えると、位相雑音を変数として)熱雑音に基づく対数尤度比に対する重み係数WNおよび位相雑音に基づく対数尤度比に対する重み係数Wφが算出されるようにしてもよい。 Note that, in Equation 8, the weighting factor WN for the log-likelihood ratio based on thermal noise and the weighting factor Wφ for the log-likelihood ratio based on phase noise are calculated based on the magnitude of the thermal noise (in other words, with the thermal noise as a variable), but the weighting factor WN for the log-likelihood ratio based on thermal noise and the weighting factor Wφ for the log-likelihood ratio based on phase noise may be calculated based on the magnitude of the phase noise (in other words, with the phase noise as a variable).

LLR算出部20の熱雑音LLR算出部21は、等化器18から出力されるベースバンド信号(受信信号)の入力を受け、前記ベースバンド信号から受信信号の同相成分xiおよび受信信号の直交成分xqを取得し、上記の数式2A乃至数式2Dに従って(bit_num)bit目の熱雑音に基づく対数尤度比LLRN(bit_num)を算出して出力する。 The thermal noise LLR calculation unit 21 of the LLR calculation unit 20 receives an input of a baseband signal (received signal) output from the equalizer 18, acquires an in-phase component x i and a quadrature component x q of the received signal from the baseband signal, and calculates and outputs a log-likelihood ratio LLR N(bit_num) based on the thermal noise of the (bit_num)th bit in accordance with the above-mentioned Formula 2A to Formula 2D.

位相雑音LLR算出部22は、等化器18から出力されるベースバンド信号(受信信号)の入力を受け、前記ベースバンド信号から受信信号の位相角度xφおよび受信信号の振幅xRを取得し、前記受信信号の振幅xRと第1の振幅閾値Rthre1や第2の振幅閾値Rthre2との大小関係も考慮したうえで、上記の数式3乃至数式6に従って(bit_num)bit目の位相雑音に基づく対数尤度比LLRφ(bit_num)を算出して出力する。 The phase noise LLR calculation unit 22 receives an input of a baseband signal (received signal) output from the equalizer 18, acquires a phase angle xφ and an amplitude xR of the received signal from the baseband signal, and calculates and outputs a log-likelihood ratio LLRφ( bit_num ) based on the phase noise of the (bit_num)th bit according to the above-mentioned Formulas 3 to 6 , while taking into consideration the magnitude relationship between the amplitude xR of the received signal and the first amplitude threshold R thre1 and the second amplitude threshold R thre2 .

熱雑音電力推定部23は、等化器18から出力されるベースバンド信号(受信信号)の入力を受け、前記ベースバンド信号に基づいて無線受信装置1における熱雑音電力を推定し、熱雑音電力の推定量を出力する。 The thermal noise power estimation unit 23 receives the baseband signal (received signal) output from the equalizer 18, estimates the thermal noise power in the wireless receiving device 1 based on the baseband signal, and outputs an estimated amount of thermal noise power.

重み係数制御部24は、等化器18から出力されるベースバンド信号(受信信号)の入力を受けるとともに、熱雑音電力推定部23から出力される熱雑音電力の推定量の入力を受け、前記ベースバンド信号および前記熱雑音電力の推定量を用いて(具体的には、熱雑音の分散Nを計算して)上記の数式8Aに従って熱雑音に基づく対数尤度比の重み係数WNを算出するとともに上記の数式8Bに従って位相雑音に基づく対数尤度比の重み係数Wφを算出して出力する。 The weighting coefficient control unit 24 receives an input of the baseband signal (received signal) output from the equalizer 18, and also receives an input of the estimated amount of thermal noise power output from the thermal noise power estimating unit 23, and uses the baseband signal and the estimated amount of thermal noise power (specifically, calculates the variance N of the thermal noise) to calculate a weighting coefficient WN of the log-likelihood ratio based on thermal noise according to the above Equation 8A, and also calculates and outputs a weighting coefficient Wφ of the log-likelihood ratio based on phase noise according to the above Equation 8B.

第1の乗算器25は、熱雑音LLR算出部21から出力される熱雑音に基づく対数尤度比LLRN(bit_num)の入力を受けるとともに、重み係数制御部24から出力される熱雑音に基づく対数尤度比の重み係数WNの入力を受け、前記熱雑音に基づく対数尤度比LLRN(bit_num)と前記熱雑音に基づく対数尤度比の重み係数WNとを乗算し、乗算した結果(即ち、WN×LLRN(bit_num))を出力する。 The first multiplier 25 receives an input of the log-likelihood ratio LLR N(bit_num) based on thermal noise output from the thermal noise LLR calculation unit 21, and also receives an input of the weighting coefficient W N of the log-likelihood ratio based on thermal noise output from the weighting coefficient control unit 24, multiplies the log-likelihood ratio LLR N(bit_num) based on thermal noise by the weighting coefficient W N of the log-likelihood ratio based on thermal noise, and outputs the multiplication result (i.e., W N × LLR N(bit_num) ).

第2の乗算器26は、位相雑音LLR算出部22から出力される位相雑音に基づく対数尤度比LLRφ(bit_num)の入力を受けるとともに、重み係数制御部24から出力される位相雑音に基づく対数尤度比の重み係数Wφの入力を受け、前記位相雑音に基づく対数尤度比LLRφ(bit_num)と前記位相雑音に基づく対数尤度比の重み係数Wφとを乗算し、乗算した結果(即ち、Wφ×LLRφ(bit_num))を出力する。 The second multiplier 26 receives an input of the log-likelihood ratio LLRφ (bit_num) based on the phase noise output from the phase noise LLR calculation unit 22, and also receives an input of the weighting coefficient Wφ of the log-likelihood ratio based on the phase noise output from the weighting coefficient control unit 24, multiplies the log-likelihood ratio LLRφ (bit_num) based on the phase noise by the weighting coefficient Wφ of the log-likelihood ratio based on the phase noise, and outputs the multiplication result (i.e., Wφ×LLRφ (bit_num) ).

加算器27は、第1の乗算器25から出力される乗算結果(即ち、WN×LLRN(bit_num))の入力を受けるとともに、第2の乗算器26から出力される乗算結果(即ち、Wφ×LLRφ(bit_num))の入力を受け、上記の数式1に従ってこれら乗算結果を加算し、加算した結果である(bit_num)bit目の対数尤度比LLRbit_num(=WN×LLRN(bit_num)+Wφ×LLRφ(bit_num))を出力する。 The adder 27 receives the multiplication result (i.e., W N ×LLR N(bit_num) ) output from the first multiplier 25 and the multiplication result (i.e., Wφ×LLRφ (bit_num) ) output from the second multiplier 26, adds these multiplication results according to the above equation 1, and outputs the sum, i.e., the log-likelihood ratio LLR bit_num (= W N ×LLR N(bit_num) + Wφ×LLRφ (bit_num )), for the (bit_num)th bit.

そして、復号部19が、LLR算出部20から出力される対数尤度比LLRbit_numの入力を受け、前記対数尤度比LLRbit_numを使用して例えばsum-product復号法に従って低密度パリティ検査復号処理を行う。 Then, the decoding unit 19 receives the log-likelihood ratio LLR bit_num output from the LLR calculation unit 20, and performs low-density parity check decoding processing using the log-likelihood ratio LLR bit_num according to, for example, the sum-product decoding method.

実施の形態に係る対数尤度比算出回路としてのLLR算出部20によれば、熱雑音に基づく対数尤度比LLRN(bit_num)と位相雑音に基づく対数尤度比LLRφ(bit_num)との相互の優先の度合いを考慮したうえで(具体的には、対数尤度比LLRN(bit_num)に重み係数WNを乗じるとともに対数尤度比LLRφ(bit_num)に重み係数Wφを乗じたうえで)これらを加算して各bitの対数尤度比LLRbit_numを算出することにより、対数尤度比の算出に熱雑音の影響に加えて位相雑音やフェージングによる分布変動の要素を考慮するようにしているので、位相雑音を含む外乱に対してロバストな低密度パリティ検査を実現することが可能となる。 According to the LLR calculation unit 20 serving as a log-likelihood ratio calculation circuit according to the embodiment, the log-likelihood ratio LLR N(bit_num) based on thermal noise and the log-likelihood ratio LLRφ (bit_num) based on phase noise are taken into consideration of the degree of mutual priority between them (specifically, the log-likelihood ratio LLR N(bit_num) is multiplied by the weighting factor W N and the log-likelihood ratio LLRφ (bit_num) is multiplied by the weighting factor Wφ), and then these are added to calculate the log-likelihood ratio LLR bit_num for each bit. This allows the calculation of the log-likelihood ratio to take into consideration factors such as phase noise and distribution fluctuation due to fading in addition to the influence of thermal noise, making it possible to realize a low-density parity check that is robust against disturbances including phase noise.

実施の形態に係る対数尤度比算出回路としてのLLR算出部20によれば、また、受信信号の位相雑音やフェージングなどによってシンボルの位相が正規分布/ガウス分布に基づいて回転・変動した際の確率分布も考慮して対数尤度比を算出するようにしているので、受信信号の位相雑音が支配的な環境下においても対数尤度比の算出精度を向上させることが可能となり、延いては、低密度パリティ検査の誤り訂正能力を向上させることが可能となる。 The LLR calculation unit 20, which serves as a log-likelihood ratio calculation circuit according to the embodiment, also calculates the log-likelihood ratio by taking into account the probability distribution when the phase of the symbol rotates or fluctuates based on a normal distribution/Gaussian distribution due to phase noise or fading of the received signal. This makes it possible to improve the calculation accuracy of the log-likelihood ratio even in an environment where phase noise of the received signal is dominant, and ultimately makes it possible to improve the error correction capability of the low-density parity check.

具体的には、図10に示すように、従来の対数尤度比の算出方法では、受信信号の熱雑音によって理想シンボル点を中心として正規分布/ガウス分布に基づいて受信信号の振幅が変動することを前提としている(同図中の破線円Cf参照)。このため、受信信号の位相雑音によってシンボルの位相が回転した際の変動(同図中の円弧矢印Fp参照)があると、受信した確率が高いと判断した信号Sfが実際の送信信号Ssとは異なってしまう。これに対して、実施の形態に係る対数尤度比算出回路としてのLLR算出部20では、受信信号の位相雑音による変動の分布を考慮するようにしているので、すなわち、受信信号の位相雑音によってシンボルが包絡線E上で変動する状況も考慮して対数尤度比を算出するようにしているので、受信信号の位相雑音によってシンボルの位相が回転した際の変動(同図中の円弧矢印Fp参照)があっても、受信した確率が高いと判断した信号が実際の送信信号Ssと一致して低密度パリティ検査の誤り訂正能力を向上させることが可能となる。 Specifically, as shown in FIG. 10, the conventional method of calculating the log likelihood ratio is based on the assumption that the amplitude of the received signal fluctuates based on a normal distribution/Gaussian distribution centered on the ideal symbol point due to thermal noise in the received signal (see the dashed circle Cf in the figure). For this reason, if there is a fluctuation when the phase of the symbol rotates due to the phase noise of the received signal (see the circular arrow Fp in the figure), the signal Sf determined to have a high probability of being received will differ from the actual transmission signal Ss. In contrast, the LLR calculation unit 20 as the log likelihood ratio calculation circuit according to the embodiment is designed to take into account the distribution of fluctuations due to the phase noise of the received signal, that is, the log likelihood ratio is calculated taking into account the situation in which the symbol fluctuates on the envelope E due to the phase noise of the received signal, so that even if there is a fluctuation when the phase of the symbol rotates due to the phase noise of the received signal (see the circular arrow Fp in the figure), the signal determined to have a high probability of being received will match the actual transmission signal Ss, making it possible to improve the error correction ability of the low-density parity check.

この発明に係る対数尤度比算出回路の有効性の検証例を下記に説明する。 An example of verifying the effectiveness of the log-likelihood ratio calculation circuit of this invention is described below.

この検証例では、熱雑音と位相雑音とが存在する環境下において従来の対数尤度比の算出方法とこの発明に係る対数尤度比算出回路との対数尤度比の算出精度を比較することを目的として、図11に示す評価系が用いられた。この検証例の評価系は、所定のサンプル信号を16QAM方式で変調する(同図中の符号31)とともに位相雑音および熱雑音を付加した(符号32,33)うえで、受信信号の熱雑音の分布に基づいて対数尤度比を算出する従来手法(符号34)と、受信信号の位相雑音も考慮して対数尤度比を算出するこの発明に係る対数尤度比算出回路(符号20)とのそれぞれの対数尤度比の算出精度を比較する系として構成された。 In this verification example, the evaluation system shown in FIG. 11 was used for the purpose of comparing the calculation accuracy of the log likelihood ratio between a conventional method for calculating the log likelihood ratio and the log likelihood ratio calculation circuit according to the present invention in an environment where thermal noise and phase noise are present. The evaluation system in this verification example was configured as a system for comparing the calculation accuracy of the log likelihood ratio between a conventional method (reference number 34) that calculates the log likelihood ratio based on the distribution of thermal noise of the received signal after modulating a predetermined sample signal using the 16QAM method (reference number 31 in the figure) and adding phase noise and thermal noise (reference numbers 32 and 33), and the log likelihood ratio calculation circuit according to the present invention (reference number 20) that calculates the log likelihood ratio while also taking into account the phase noise of the received signal.

また、この検証例の評価条件は下記のように設定された。
変調方式:16QAM方式
搬送波対雑音比(CNR:Carrier‐Noise Ratio の略):15~25dB
位相雑音レベル:-60dBc(1kHzオフセットにおける値)
QAM方式のシンボル間間隔Sd:2
優先調整係数α:0.125
同等調整係数β:100
The evaluation conditions for this verification example were set as follows:
Modulation method: 16QAM method Carrier-to-noise ratio (CNR: Carrier-Noise Ratio): 15 to 25 dB
Phase noise level: -60 dBc (at 1 kHz offset)
Symbol interval S d in QAM system: 2
Priority adjustment coefficient α: 0.125
Equivalent adjustment coefficient β: 100

ここで、対数尤度比は、送信bitが0である確率が高いときに正の値をとり、送信bitが1である確率が高いときに負の値をとる。このことを利用し、実際の送信bitと従来手法(図9中の符号34)で算出した対数尤度比の符号とを比較して符号が誤っている回数を計数する(符号35)とともに、実際の送信bitとこの発明に係る対数尤度比算出回路(符号20)で算出した対数尤度比の符号とを比較して符号が誤っている回数を計数した(符号36)。 The log-likelihood ratio takes a positive value when the probability that the transmitted bit is 0 is high, and takes a negative value when the probability that the transmitted bit is 1 is high. Using this, the actual transmitted bit is compared with the sign of the log-likelihood ratio calculated by the conventional method (reference number 34 in FIG. 9) to count the number of times the sign is incorrect (reference number 35), and the actual transmitted bit is compared with the sign of the log-likelihood ratio calculated by the log-likelihood ratio calculation circuit of this invention (reference number 20) to count the number of times the sign is incorrect (reference number 36).

図11に示す評価系による結果として、図12に示すように、各搬送波対雑音比において、この発明に係る対数尤度比算出回路の方が符号の誤り率が小さいことが確認された。また、搬送波対雑音比が高くなって位相雑音が支配的になるほど、この発明に係る対数尤度比算出回路による改善率が大きくなることが確認された。この結果から、この発明に係る対数尤度比算出回路によれば、従来の対数尤度比の算出方法と比べて、符号の誤り率が低減することが確認された。 As a result of the evaluation system shown in FIG. 11, it was confirmed that the log-likelihood ratio calculation circuit of the present invention had a smaller code error rate at each carrier-to-noise ratio, as shown in FIG. 12. It was also confirmed that the higher the carrier-to-noise ratio and the more dominant the phase noise, the greater the improvement rate achieved by the log-likelihood ratio calculation circuit of the present invention. From these results, it was confirmed that the code error rate is reduced by the log-likelihood ratio calculation circuit of the present invention compared to the conventional log-likelihood ratio calculation method.

以上、この発明の実施の形態について説明したが、具体的な構成は、上記の実施の形態に限られるものではなく、この発明の要旨を逸脱しない範囲の設計の変更等があっても、この発明に含まれる。 The above describes an embodiment of the present invention, but the specific configuration is not limited to the above embodiment, and even if there are design changes within the scope of the invention that do not deviate from the gist of the invention, they are still included in the invention.

具体的には、上記の実施の形態ではこの発明に係る対数尤度比算出回路が図1に概略構成を示す無線受信装置1にLLR算出部20として組み込まれるようにしているが、この発明に係る対数尤度比算出回路が組み込まれ得る無線装置の構成は図1に概略構成を示す無線受信装置1に限定されるものではなく、この発明に係る対数尤度比算出回路が他の構成の無線装置に組み込まれるようにしてもよい。 Specifically, in the above embodiment, the log-likelihood ratio calculation circuit according to the present invention is incorporated as an LLR calculation unit 20 in a wireless receiving device 1 whose schematic configuration is shown in FIG. 1, but the configuration of a wireless device in which the log-likelihood ratio calculation circuit according to the present invention can be incorporated is not limited to the wireless receiving device 1 whose schematic configuration is shown in FIG. 1, and the log-likelihood ratio calculation circuit according to the present invention may be incorporated in a wireless device of another configuration.

また、上記の実施の形態では熱雑音に基づく対数尤度比LLRN(bit_num)が上記の数式2A乃至数式2Dに従って算出されるようにしているが、熱雑音に基づく対数尤度比LLRN(bit_num)の算出式/算出方法は数式2A乃至数式2Dに限定されるものではなく、また、上記の実施の形態では位相雑音に基づく対数尤度比LLRφ(bit_num)が上記の数式3乃至数式6に従って算出されるようにしているが、位相雑音に基づく対数尤度比LLRφ(bit_num)の算出式/算出方法は数式3乃至数式6に限定されるものではない。すなわち、この発明の要点は熱雑音に基づく対数尤度比LLRN(bit_num)と位相雑音に基づく対数尤度比LLRφ(bit_num)との相互の優先の度合いを考慮したうえで(具体的には、対数尤度比LLRN(bit_num)に重み係数WNを乗じるとともに対数尤度比LLRφ(bit_num)に重み係数Wφを乗じたうえで)これらを加算して各bitの対数尤度比LLRbit_numを算出することであり、熱雑音に基づく対数尤度比LLRN(bit_num)や位相雑音に基づく対数尤度比LLRφ(bit_num)の算出式/算出方法を含むその他の構成は特定の構成には限定されない。 In addition, in the above embodiment, the log-likelihood ratio LLR N(bit_num) based on thermal noise is calculated according to the above Formula 2A to Formula 2D, but the calculation formula/method of the log-likelihood ratio LLR N(bit_num) based on thermal noise is not limited to Formula 2A to Formula 2D, and in the above embodiment, the log-likelihood ratio LLRφ (bit_num) based on phase noise is calculated according to the above Formula 3 to Formula 6, but the calculation formula/method of the log-likelihood ratio LLRφ (bit_num) based on phase noise is not limited to Formula 3 to Formula 6. That is, the gist of the present invention is to calculate the log-likelihood ratio LLR bit_num for each bit by taking into consideration the degree of mutual priority between the log-likelihood ratio LLR N (bit_num) based on thermal noise and the log-likelihood ratio LLRφ (bit_num) based on phase noise (specifically, by multiplying the log-likelihood ratio LLR N (bit_num) by a weighting coefficient W N and multiplying the log-likelihood ratio LLRφ (bit_num) by a weighting coefficient Wφ) and adding these, and other configurations including the calculation formula/method of the log-likelihood ratio LLR N(bit_num) based on thermal noise and the log-likelihood ratio LLRφ (bit_num) based on phase noise are not limited to specific configurations.

1 無線受信装置
10 アンテナ
11 チャネルフィルタ
12 局部発振器
13 ミキサ
14 自動利得制御部
15 A/D変換器
16 デジタル直交検波部
17 ロールオフフィルタ
18 等化器
19 復号部
20 LLR算出部
21 熱雑音LLR算出部
22 位相雑音LLR算出部
23 熱雑音電力推定部
24 重み係数制御部
25 第1の乗算器
26 第2の乗算器
27 加算器
REFERENCE SIGNS LIST 1 Radio receiving device 10 Antenna 11 Channel filter 12 Local oscillator 13 Mixer 14 Automatic gain control section 15 A/D converter 16 Digital quadrature detection section 17 Roll-off filter 18 Equalizer 19 Decoding section 20 LLR calculation section 21 Thermal noise LLR calculation section 22 Phase noise LLR calculation section 23 Thermal noise power estimation section 24 Weighting coefficient control section 25 First multiplier 26 Second multiplier 27 Adder

Claims (3)

熱雑音に基づく対数尤度比と位相雑音に基づく対数尤度比とのそれぞれに重み係数を乗じたうえで加算して対数尤度比を算出する対数尤度比算出回路であって
前記位相雑音に基づく対数尤度比を、
送信側において多値数が16の直角位相振幅変調方式で変調された4bitの受信信号のうち、
理想シンボル点の位相角度に応じて0になるか1になるかが区別されているbitについては、
前記受信信号の位相角度を用いて、位相角度に応じて0になる確率密度分布と1になる確率密度分布とに基づいて算出し、
振幅に応じて0になるか1になるかが区別されている理想シンボル点(「振幅区別シンボル点」と呼ぶ)と位相角度に応じて0になるか1になるかが区別されている理想シンボル点(「位相区別シンボル点」と呼ぶ)とに分けられるbitについては、
前記振幅区別シンボル点と前記位相区別シンボル点とのうちのどちらであるかを前記受信信号の振幅に基づいて判断したうえで、
前記振幅区別シンボル点について、前記受信信号の振幅を用いて、振幅に応じて0になる確率密度分布と1になる確率密度分布とに基づいて算出し、
前記位相区別シンボル点について、前記受信信号の位相角度を用いて、位相角度に応じて0になる確率密度分布と1になる確率密度分布とに基づいて算出する、
ことを特徴とする対数尤度比算出回路。
a log likelihood ratio calculation circuit that calculates a log likelihood ratio by multiplying a log likelihood ratio based on thermal noise and a log likelihood ratio based on phase noise by a weighting factor and then adding the weighting factors,
The log-likelihood ratio based on the phase noise is
Of the 4-bit received signals modulated by quadrature amplitude modulation with a multi-level of 16 on the transmitting side,
For bits that are differentiated as 0 or 1 depending on the phase angle of the ideal symbol point,
using a phase angle of the received signal, calculating based on a probability density distribution that becomes 0 and a probability density distribution that becomes 1 according to the phase angle;
Regarding bits that can be divided into ideal symbol points that are distinguished as being 0 or 1 depending on the amplitude (called "amplitude-distinguishing symbol points") and ideal symbol points that are distinguished as being 0 or 1 depending on the phase angle (called "phase-distinguishing symbol points"),
determining whether the symbol point is the amplitude-distinguishing symbol point or the phase-distinguishing symbol point based on the amplitude of the received signal;
calculating the amplitude-distinguishing symbol point based on a probability density distribution that becomes 0 and a probability density distribution that becomes 1 according to the amplitude using the amplitude of the received signal;
calculating the phase-distinguishing symbol point based on a probability density distribution that becomes 0 and a probability density distribution that becomes 1 according to the phase angle using a phase angle of the received signal;
A log-likelihood ratio calculation circuit comprising:
前記理想シンボル点の位相角度に応じて0になるか1になるかが区別されているbitである1bit目について下記の数式1に従って位相雑音に基づく対数尤度比を算出するとともに3bit目について下記の数式3に従って位相雑音に基づく対数尤度比を算出し、
前記振幅区別シンボル点と前記位相区別シンボル点とに分けられるbitである2bit目について下記の数式2に従って位相雑音に基づく対数尤度比を算出するとともに4bit目について下記の数式4に従って位相雑音に基づく対数尤度比を算出する(但し、xR≧Rthre1 または xR≦Rthre2 のときに数式2Aおよび数式4Aが用いられ、Rthre2<xR<Rthre1 のときに数式2Bおよび数式4Bが用いられる)、
ここに、
xφ:受信信号の位相角度
R:受信信号の振幅
φi:理想シンボル点の位相角度(但し、φの添字i=0,1,2,・・・,11)
i:理想シンボル点の振幅(但し、Rの添字i=0,1,2)
σ2:雑音分散
thre1:第1の振幅閾値
thre2:第2の振幅閾値
ことを特徴とする請求項に記載の対数尤度比算出回路。
A log likelihood ratio based on phase noise is calculated for a first bit, which is a bit that is distinguished as being 0 or 1 depending on the phase angle of the ideal symbol point, according to the following Equation 1, and a log likelihood ratio based on phase noise is calculated for a third bit, according to the following Equation 3,
A log likelihood ratio based on phase noise is calculated for the second bit, which is a bit divided into the amplitude-distinguishing symbol point and the phase-distinguishing symbol point, according to the following Equation 2, and a log likelihood ratio based on phase noise is calculated for the fourth bit, according to the following Equation 4 (wherein Equation 2A and Equation 4A are used when xRRthre1 or xRRthre2 , and Equation 2B and Equation 4B are used when Rthre2 < xR < Rthre1 ).
Here,
xφ: Phase angle of the received signal xR : Amplitude of the received signal φi : Phase angle of the ideal symbol point (where the subscript i of φ is 0, 1, 2, ..., 11)
R i : Amplitude of the ideal symbol point (where the subscript i of R = 0, 1, 2)
2. The log-likelihood ratio calculation circuit according to claim 1 , wherein σ 2 is a noise variance, R thre1 is a first amplitude threshold, and R thre2 is a second amplitude threshold.
請求項1または2のいずれか1項に記載の対数尤度比算出回路を備える、
ことを特徴とする無線受信装置。
A log-likelihood ratio calculation circuit according to claim 1 or 2 ,
A radio receiving device comprising:
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WO2010140448A1 (en) 2009-06-03 2010-12-09 日本電気株式会社 Likelihood value calculation device, likelihood value calculation method, and radio system
WO2018116411A1 (en) 2016-12-21 2018-06-28 日本電気株式会社 Modulation method, decoding method, modulation device and demodulation device

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WO2010140448A1 (en) 2009-06-03 2010-12-09 日本電気株式会社 Likelihood value calculation device, likelihood value calculation method, and radio system
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Toshiaki Koike-Akino, et al.,Phase noise-robust LLR calculation with linear/bilinear transform for LDPC-coded coherent communications,2015 Conference on Lasers and Electro-Optics (CLEO)[online],2015年08月13日, [retrieved on 2024.10.28], Retrieved from the Internet: <URL: https://ieeexplore.ieee.org/stamp/stamp.jsp?tp=&arnumber=7184331>,<DOI: 10.1364/CLEO_SI.2015.SW1M.3>

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