TWI401900B - Method for partitioning a period according to noise characteristics - Google Patents
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Description
本發明是有關於一種在通訊系統中的雜訊估測方法,且特別是有關於一種依據雜訊特性分割雜訊之週期的方法。The present invention relates to a method for estimating noise in a communication system, and more particularly to a method for dividing a period of noise according to a noise characteristic.
電力線早在多年前就已是分布相當廣泛的線路資源,分布於家庭、公司、學校等等的各種機關,並且由於近年來通訊技術的進步,所以目前已發展出使用電力線來傳輸資料,稱之為電力線通訊(Power Line Communication)。而電力線通訊的技術主要是將所欲傳輸之資料調變為一高頻訊號,再將高頻訊號與低頻的電力訊號一起耦合到電力線中,就可同時傳輸資料與電力。The power line has been a widely distributed line resource many years ago, distributed in various institutions such as families, companies, schools, etc., and due to the advancement of communication technology in recent years, the use of power lines to transmit data has been developed. For Power Line Communication. The technology of power line communication mainly transforms the data to be transmitted into a high-frequency signal, and then couples the high-frequency signal with the low-frequency power signal into the power line to transmit data and power simultaneously.
在目前利用電力線傳輸的通道,由於本身已有頻率為50~60Hz的交流電在電力線中傳輸,而交流電為一週期性的弦波。因此,造成電力線傳輸的通道中雜訊也將週期性的出現,稱為循環平穩雜訊(cyclostationary noise)。In the current channel using power line transmission, since the existing alternating current frequency of 50~60 Hz is transmitted in the power line, the alternating current is a periodic sine wave. Therefore, the noise in the channel causing the power line transmission will also appear periodically, which is called cyclostationary noise.
然而,在目前的電力線通訊的技術中,雖已觀察出此傳輸通道之中之雜訊週期性地出現,但並未利用此種特性,在週期內區分多個時間區段來對應不同的雜訊特性,並利用不同的雜訊特性調整傳輸之位元率(bit rate)或是傳輸訊號之能量。因此,當在週期內部分時間區段中,由於雜訊過大,將造成所傳輸信號受到過多的雜訊干擾而無法還原原始之資料。However, in the current power line communication technology, although the noise in the transmission channel has been observed to occur periodically, this feature is not utilized, and multiple time segments are distinguished in the cycle to correspond to different impurities. The characteristics of the signal, and use different noise characteristics to adjust the bit rate of the transmission or the energy of the transmitted signal. Therefore, when the noise is too large in part of the time period, the transmitted signal will be subject to excessive noise interference and the original data cannot be restored.
本發明的目的就是在提供一種依據雜訊特性分割循環平穩雜訊之週期的方法,透過偵測雜訊特性的變化,將每個週期分割為不同的時間區段。SUMMARY OF THE INVENTION It is an object of the present invention to provide a method for segmenting a period of cyclically stationary noise based on noise characteristics, and dividing each period into different time segments by detecting changes in noise characteristics.
本發明提出一種依據雜訊特性分週期的方法,包括:提供一週期;當傳輸通道為無封包的狀態時,統計第i週期內的多個雜訊特性變化值;在第i週期中,找出些雜訊特性變化值的最大值及其對應的第一時間點;利用第一時間點,將週期分割為第一時間區段與第二時間區段。The invention provides a method for dividing the period according to the characteristics of the noise, comprising: providing a period; when the transmission channel is in a state of no packet, counting a plurality of noise characteristic changes in the i-th cycle; in the i-th cycle, looking for A maximum value of the noise characteristic change value and a corresponding first time point are obtained; and the first time point is used to divide the period into the first time segment and the second time segment.
本發明透過偵測雜訊能量的變化以及雜訊在頻譜上之變化,將一週期分割為多個時間區段,並且讓每個時間區段對應到一雜訊之特性,以讓收發端能夠得知此時雜訊的特性。因此,收發端能夠依據此時的雜訊特性,適當地調整例如傳輸之位元率或傳輸信號之能量大小。The invention divides a cycle into a plurality of time segments by detecting a change in the noise energy and a change in the spectrum of the noise, and allows each time segment to correspond to a characteristic of a noise, so that the transceiver can Know the characteristics of the noise at this time. Therefore, the transceiver can appropriately adjust, for example, the bit rate of the transmission or the energy of the transmission signal according to the noise characteristics at this time.
為讓本發明之上述和其他目的、特徵和優點能更明顯易懂,下文特舉較佳實施例,並配合所附圖式,作詳細說明如下。The above and other objects, features and advantages of the present invention will become more <RTIgt;
由於在目前的習知技術中,並未利用傳輸通道之中之雜訊週期性地出現的特性,在週期內區分多個時間區段來對應不同的雜訊特性,導致當雜訊過大時傳輸資料的遺失。因此,本發明提出一種依據雜訊特性分割循環平穩雜訊之週期的方法,能夠依據雜訊的能量與雜訊之頻譜,將一週期分割為多個時間區段,以讓後端電路能夠依據時間區段,來適當地調整傳輸之位元率或是傳輸訊號之能量。In the prior art, the characteristics that periodically occur in the transmission channel are not utilized, and multiple time segments are distinguished in the cycle to correspond to different noise characteristics, resulting in transmission when the noise is too large. Loss of information. Therefore, the present invention provides a method for dividing the period of the cyclostationary noise according to the noise characteristic, which can divide the period into a plurality of time segments according to the energy of the noise and the spectrum of the noise, so that the back-end circuit can be based on The time zone is used to properly adjust the bit rate of the transmission or the energy of the transmitted signal.
以下將提出本發明實施例之依據雜訊特性分割循環平穩雜訊之週期的方法,而在說明本實施之前,先假設傳輸通道為電力線傳輸通道,但並不限制本發明。而在電力線中,由於已存在有一週期之交流電,此週期稱為交流電力線週期(Mains Cycle或AC Line Cycle),因而造成電力線傳輸通道中之雜訊週期性的出現,也就是說,在本實施例中,傳輸通道中的雜訊例如為循環平穩雜訊。接著,假設本實施例中,此交流電的頻率50Hz,而此交流電力線週期為0.02sec。並且,假設每個交流電力線週期傳送200個符元,而每個符元時間為0.0001sec。為了簡化說明本實施例,以下交流電力線週期皆簡稱為週期,其長度等於循環平穩雜訊之週期。Hereinafter, a method for dividing the period of the cyclosynchronous noise according to the noise characteristic according to the embodiment of the present invention will be proposed. Before the present embodiment is explained, the transmission channel is assumed to be a power line transmission channel, but the present invention is not limited. In the power line, since there is already one cycle of alternating current, this cycle is called the alternating current line cycle (Mains Cycle or AC Line Cycle), thus causing the occurrence of noise in the power line transmission channel periodically, that is, in this implementation. In the example, the noise in the transmission channel is, for example, a cyclostationary noise. Next, it is assumed that in the present embodiment, the frequency of the alternating current is 50 Hz, and the period of the alternating current power line is 0.02 sec. Also, assume that each AC power line periodically transmits 200 symbols, and each symbol time is 0.0001 sec. In order to simplify the description of the embodiment, the following AC power line periods are simply referred to as periods, and the length thereof is equal to the period of the cyclic stationary noise.
此外,假設在電力線傳輸通道中,資料是以封包之形式傳輸,因此,通道為無封包的狀態時,接收端所接收到之訊號為通道中之雜訊。並且,假設此方法適用於一收發器中,而此收發器能夠偵測出通道中是否有封包正在傳遞。為了方便說明本實施例,本實施例皆假設通道為無封包狀態。然而,本領域據通常知識者應當可推知,由於收發器能夠持續地偵測通道中是否有封包在傳遞,當通道傳遞封包時,收發器將暫時停止進行此方法,並等到通道中沒有傳遞封包時,再繼續開始進行此方法。In addition, it is assumed that in the power line transmission channel, the data is transmitted in the form of a packet. Therefore, when the channel is in a non-packet state, the signal received by the receiving end is the noise in the channel. Also, assume that this method is suitable for use in a transceiver that can detect if a packet is being transmitted in the channel. For convenience of description of the embodiment, this embodiment assumes that the channel is in a no-packet state. However, those skilled in the art should be able to infer that since the transceiver can continuously detect whether a packet is being transmitted in the channel, when the channel transmits the packet, the transceiver will temporarily stop the method and wait until there is no packet in the channel. Then continue to start this method.
另外,假設此收發器應用於正交分頻多工(Orthogonal Frequency-Division Multiplexing,OFDM)系統中,因此,收 發器中包含一傅立葉轉換單元,並假設每個OFDM符元包含1536個子載波,透過傅立葉轉換單元可進行1536點之快速傅立葉轉換,以得到接收符元在每個子載波頻率上之分量。接下來,將以上述所假設的環境,來說明本實施例所提出之依據雜訊特性分割週期的方法,但是上述所假設的環境並不能用以限制本發明,本發明仍可適用於其他種類之通訊環境。In addition, it is assumed that the transceiver is applied to an Orthogonal Frequency-Division Multiplexing (OFDM) system. The transmitter includes a Fourier transform unit, and assuming that each OFDM symbol contains 1536 subcarriers, a fast Fourier transform of 1536 points can be performed by the Fourier transform unit to obtain a component of the received symbol at each subcarrier frequency. Next, the method according to the embodiment of the present invention for determining the segmentation period of the noise characteristic will be described. However, the above-mentioned assumed environment cannot be used to limit the present invention, and the present invention can be applied to other types. Communication environment.
圖1繪示為本發明實施例之依據雜訊特性分割週期的方法步驟流程圖。請參照圖1,開始依據雜訊特性分割週期(步驟S100),並提供一符元紀錄表(步驟S102)。而在本實施例中,此符元紀錄表用以紀錄每個時間區段的起始與結束時間點。並由於每個時間區段將可能對應到不同的雜訊型態,因此,符元紀錄表中還紀錄了每個時間區段所對應的雜訊型態索引,而不同的雜訊型態索引將具有不同的雜訊型態。此時,由於尚未開始分割週期,因此,整個交流電力線週期可視為同一時間區段,而在此時間區段內雜訊皆視為相同的雜訊型態。FIG. 1 is a flow chart showing the steps of a method for dividing a cycle according to a noise characteristic according to an embodiment of the present invention. Referring to FIG. 1, the segmentation period according to the noise characteristic is started (step S100), and a symbol record table is provided (step S102). In this embodiment, the symbol record table is used to record the start and end time points of each time segment. And because each time segment will probably correspond to different noise patterns, the symbol record table also records the noise type index corresponding to each time segment, and different noise type indexes. Will have different noise patterns. At this time, since the segmentation period has not yet started, the entire AC power line cycle can be regarded as the same time zone, and the noise is regarded as the same noise type in this time zone.
接下來,收發器在第i-1個週期接收傳輸通道中之符元(步驟S105),其中符元為經過取樣後的接收信號,i為一正整數。而在本實施例中,並未限定i之值,也就是說,本實施例之分割週期的方法可由任意時間週期開始操作。由於上述已假設此時通道為無封包的狀態,因此所接收到的符元內之訊號皆為雜訊。並且,為了方便說明本實施例, 以下將週期內的每個符元表示為r (s ),其中s 為符元時間索引(symbol index),且由於每個週期內包含200個符元,因此s 介於0~199之間。Next, the transceiver receives the symbols in the transmission channel in the i-1th cycle (step S105), wherein the symbol is the sampled received signal, and i is a positive integer. In the present embodiment, the value of i is not limited, that is, the method of dividing the period of the embodiment can be started by any time period. Since the above assumption is made that the channel is in a state of no packet, the signals in the received symbols are all noise. Moreover, for convenience of description of the present embodiment, each symbol in the period is expressed as r ( s ), where s is a symbol index, and since each period contains 200 symbols, s is between 0 and 199.
之後,收發器利用傅立葉轉換單元將接收之符元轉至頻域(步驟S110)。而在本實施例中,假設每個符元r (s )經過取樣後,皆包含1536個取樣點,而在步驟S110中,將1536個取樣點經過1536點的快速傅立葉轉換後,將得到1536個子載波頻率分量。而為了方便說明本實施例,每個符元r (s )經過取樣與快速傅立葉轉換皆表示為R s (k ),而R s (k )=FFT [r (s )],其中k 為子載波索引,且k 介於0~1535。Thereafter, the transceiver uses the Fourier transform unit to transfer the received symbols to the frequency domain (step S110). In this embodiment, it is assumed that each symbol r ( s ) is sampled and contains 1536 sampling points, and in step S110, 1536 sampling points are subjected to fast FFT conversion at 1536 points, and 1536 is obtained. Subcarrier frequency components. For convenience of description of the present embodiment, each symbol r ( s ) is sampled and fast Fourier transformed is represented as R s ( k ), and R s ( k )= FFT [ r ( s )], where k is a sub- Carrier index, and k is between 0 and 1535.
接下來,利用1536個子載波頻率分量,統計i-1個週期內,每個符元的雜訊特性變化值(步驟S120),表示為diffOfDist (s )。在本實施例中,步驟S120包括多個子步驟,並繪示於圖2中。圖2繪示為步驟S120之子步驟的流程圖。Next, using 1536 subcarrier frequency components, the noise characteristic change value of each symbol in i-1 cycles is counted (step S120), which is expressed as diffOfDist ( s ). In this embodiment, step S120 includes a plurality of sub-steps and is illustrated in FIG. FIG. 2 is a flow chart showing the sub-steps of step S120.
請參考圖2,首先,將傳輸通道分為多個子頻帶(步驟S210),也就是將相鄰的子載波頻率分為相同子頻帶,而在本實施例中,以每64個連續的子載波視為相同的子頻帶,因此,1536個子載波分為24個子頻帶。之後,提供一記憶體(步驟S215),此記憶體可分為24個區塊,以分別對應24個子頻帶。而在每個區塊中儲存一參考子頻帶雜訊能量,而每個區塊中的參考子頻帶雜訊能量分別表示一個子頻帶能量的平均值,而參考子頻帶雜訊能量之計算方法將 在之後的步驟中有詳盡的描述。Referring to FIG. 2, first, the transmission channel is divided into a plurality of sub-bands (step S210), that is, the adjacent sub-carrier frequencies are divided into the same sub-band, and in this embodiment, every 64 consecutive sub-carriers It is regarded as the same sub-band, and therefore, 1536 sub-carriers are divided into 24 sub-bands. Thereafter, a memory is provided (step S215), and the memory can be divided into 24 blocks to correspond to 24 sub-bands, respectively. And storing a reference sub-band noise energy in each block, and the reference sub-band noise energy in each block respectively represents the average value of the energy of one sub-band, and the calculation method of the reference sub-band noise energy will be A detailed description is given in the following steps.
在之後的步驟中,每個符元皆進行相同的差值運算,因此以下的步驟以第s
個符元為例。接下來,計算第s
個符元中,每個子頻帶的能量(步驟S220)。以第b
個子頻帶為例,其子頻帶的能量表示為bandEnergy
(b
),而b
為一整數,且介於0~23之間,而第b
子頻帶的能量之運算式例如為:
在計算出子頻帶的能量之後,將每個子頻帶的能量減去其所對應的參考子頻帶雜訊能量,得到每個子頻帶能量差值(步驟S225)。以第b 個子頻帶為例,其子頻帶能量差值之運算式例如為bandEnergy (b )-noiseTemplate (b ),其中noiseTemplate (b )為第b 子頻帶之參考子頻帶雜訊能量。After calculating the energy of the sub-band, the energy of each sub-band is subtracted from the reference sub-band noise energy corresponding thereto, and the energy difference value of each sub-band is obtained (step S225). Taking the b- th sub-band as an example, the calculation formula of the sub-band energy difference is, for example, bandEnergy ( b ) -noiseTemplate ( b ), where noiseTemplate ( b ) is the reference sub-band noise energy of the b - th sub-band.
接下來,累加每個子頻帶能量差值,作為第s
個符元頻帶能量差值(步驟S230)。以第b
個子頻帶為例,上述步驟S225與S230之運算式例如為:
之後,計算第s
個符元能量(步驟S235)。其計算的方法,可以是累加每個子頻帶的能量bandEnergy
(b
),或是,累加每個以載波頻率上之分量,其運算式例如為:
接下來,將第s 個符元能量減去第(s -C )個符元能量,得到第s 個符元能量差值(步驟S240)。符元能量差值的物理意義為第s 個符元能量與其之前C 個符元時間的符元能量之差異,而其運算式例如為symbolEnergy (s )-symbolEnergy (s -C )。其中,C 為自然數,其值可由收發器之設計者預先設定,而其物理意義為雜訊特性變化所需的暫態時間長度。Subsequently, the s-th symbol energy subtracting (s - C) a symbol energy to obtain the s-th symbol energy difference values (step S240). Physical meaning symbol energy difference is the s-th symbol energy difference between the energy of the symbol one symbol C before its time, and the calculation formula, for example symbolEnergy (s) - symbolEnergy (s - C). Where C is a natural number, the value of which can be preset by the designer of the transceiver, and its physical meaning is the length of transient time required for the change of the noise characteristic.
之後,累加第(s -C )個符元頻帶能量差值至第s 個符元頻帶能量差值後除以C ,得到第s 個平均頻帶能量差值(步驟S245),其運算式可表示為。而平均頻帶能量差值的物理意義為從(s -C )~s 符元時間內每個符元頻譜變化的平均。Thereafter, the accumulation section (s - C) a symbol energy difference of the band to the s-th symbol energy difference divided by the band C, giving the average energy difference between the s-th frequency band (step S245), the calculation may be represented by the formula for . The physical meaning of the average band energy difference is the average of the spectral changes of each symbol from ( s - C ) to s symbol time.
然後,將第s
個符元能量差值乘上第一比例常數A
加上(1-第一比例常數A
)乘上第s
個平均頻帶能量差值,得到
第s
個雜訊特性變化值(步驟S250),表示為diffOfDist
(s
),其運算式例如表示如下:
接下來,利用步驟S220所計算出的子頻帶的能量bandEnergy (b ),更新記憶體中的24個區塊內的參考子頻帶雜訊能量noiseTemplate (b )(步驟S255)。而更新的方法例如利用一自迴歸(Auto Regressive)運算,以第b 子頻帶為例,其參考子頻帶雜訊能量noiseTemplste (b )計算如下所述:noiseTemplate (b )=α*bandEnergy +(1-α)*noiseTemplate' (b )其中,noiseTemplate' (b )為記憶體中所讀取之參考子頻帶雜訊能量,noiseTemplate (b )為經過自迴歸運算後所更新之參考子頻帶雜訊能量。而α為自迴歸係數,其值可由設計者自行調整,以決定參考子頻帶雜訊能量收斂之快慢。由上述之數學式可觀查出,在本方法還沒開始進行之前,參考子頻帶雜訊能量需要一初始值,而此值可由設計者自行設定。而在每個符元中,記憶體中的24個區塊內分別儲存之參考子頻帶雜訊能量皆會被更新一次。因此,接下來的步 驟,將分別更新過的參考子頻帶雜訊能量noiseTemplate(b) 分別儲存至所對應的記憶體中之區塊(步驟S260)。Next, the reference sub-band noise energy noiseTemplate ( b ) in the 24 blocks in the memory is updated by using the energy bandEnergy ( b ) of the sub-band calculated in step S220 (step S255). The updated method uses, for example, an Auto Regressive operation, taking the b - th sub-band as an example, and the reference sub-band noise energy noiseTemplste ( b ) is calculated as follows: noiseTemplate ( b )=α* bandEnergy +(1 -α)* noiseTemplate' ( b ) where noiseTemplate' ( b ) is the reference sub-band noise energy read in the memory, and noiseTemplate ( b ) is the reference sub-band noise energy updated after autoregressive operation . And α is an autoregressive coefficient, and its value can be adjusted by the designer to determine how fast the reference sub-band noise energy converges. It can be seen from the above mathematical formula that the reference sub-band noise energy needs an initial value before the method has begun yet, and this value can be set by the designer. In each symbol, the reference sub-band noise energy stored in each of the 24 blocks in the memory is updated once. Therefore, in the next step, the separately updated reference sub-band noise energy noiseTemplate (b) is separately stored in the corresponding block in the memory (step S260).
在更新參考子頻帶雜訊能量後,利用步驟S235所計算出的符元能量symbolEnergy (s ),更新一參考雜訊能量(步驟S260),表示為noiseTemplatePower 。此參考雜訊能量noiseTemplatePower 在上述之實施例中並未描述,而其主要之用途將在本實施例之後描述。After updating the reference sub-band noise energy, a reference noise energy (step S260) is updated by using the symbol energy symbolEnergy ( s ) calculated in step S235, and is represented as noiseTemplatePower . This reference noise energy noiseTemplatePower is not described in the above embodiments, and its main use will be described later in this embodiment.
而在本實施例中參考雜訊能量例如儲存於暫存器中。每個符元s
在步驟S235中,皆計算出一symbolEnergy
(s
),在步驟S260中,將更新此暫存器內的參考雜訊能量。更新的方法例如相同於上述步驟S255,利用一自迴歸運算來更新參考雜訊能量,而其計算如下所述:
接著,請回頭參考圖1,在統計出第i-1週期內,每個符元的雜訊特性變化值diffOfDist (s )之後,找出整個i-1週期內,所有符元的雜訊特性變化值的最大值,以及對應的時間點(步驟S130),而上述最大值為多個雜訊特性變化值中之全域最大值(global maximum)。舉例來說,在步驟S120中,每個符元所計算出之符元能量與雜訊特性變化值如圖3所示。Next, please refer back to Figure 1. After counting the noise variation value of each symbol in the i- 1th period, after the diffOfDist ( s ), find the noise characteristics of all symbols in the entire i-1 period. The maximum value of the change value, and the corresponding time point (step S130), and the maximum value is the global maximum of the plurality of noise characteristic change values. For example, in step S120, the symbol energy and the noise characteristic change value calculated by each symbol are as shown in FIG. 3.
圖3(a)繪示為每個符元所對應之符元能量。圖3(b)繪示為每個符元所對應之雜訊特性變化值。圖3(c)繪示為週期內之時間分割及對應的雜訊型態。圖3之(a)、(b)、(c)之橫座標皆為符元時間索引,而圖3(a)之縱座標為符元能量,圖3(b)之縱座標為雜訊特性變化值,圖3(c)之縱座標為雜訊型態索引,其中,雜訊型態索引將在之後的步驟中詳述。Figure 3 (a) shows the symbol energy corresponding to each symbol. FIG. 3(b) illustrates the change in the noise characteristic corresponding to each symbol. Figure 3 (c) shows the time division and corresponding noise patterns in the period. The abscissas of (a), (b), and (c) of Figure 3 are all symbolic time indices, while the ordinate of Figure 3(a) is the symbol energy, and the ordinate of Figure 3(b) is the noise characteristic. The change value, the ordinate of Figure 3(c) is the noise type index, where the noise pattern index will be detailed in the following steps.
圖3(b)中,雜訊特性變化值之全域最大值出現在符元時間s =103之時間點,在此,將s =103之時間點表示為TG (i-1),也就是在第i-1週期內所找出的全域最大值所對應的時間點,因此,在步驟S130中,所找出之全域最大值出現的時間點TG (i-1)為s =103。而由於此時尚未分割週期,因此,在圖3(c)中雜訊型態索引為一直線。In Fig. 3(b), the global maximum value of the change value of the noise characteristic occurs at the time point of the symbol time s = 103, where the time point of s = 103 is expressed as T G (i-1), that is, The time point corresponding to the global maximum value found in the i-1th period, therefore, in step S130, the time point T G (i-1) at which the found global maximum value appears is s = 103. Since the period has not been divided at this time, the noise pattern index is a straight line in FIG. 3(c).
接下來,請回頭參考圖1,在第i週期內,統計每個符元的雜訊特性變化值(步驟S135)。而其統計之方法,如圖2中所述,故不再詳加贅述。Next, referring back to FIG. 1, in the i-th cycle, the noise characteristic change value of each symbol is counted (step S135). The method of its statistics, as described in Figure 2, is not described in detail.
接著,在計算出每個符元的雜訊特性變化值之後,將在時間點TG (i-1)前後一範圍內,找出雜訊特性變化值之區域最大值(local maximum),及其對應的時間點(步驟S140)。在本實施例中,上述範圍例如為20個符元時間,也就是說步驟S140將尋找s =83~s =123之間雜訊特性變化值之區域最大值。在此,為了方便說明本實施例,在第i週期找出的區域最大值對應之時間點表示為TL (i)。Then, after calculating the change value of the noise characteristic of each symbol, the local maximum value of the variation value of the noise characteristic is found within a range before and after the time point T G (i-1), and Its corresponding time point (step S140). In the present embodiment, the above range is, for example, 20 symbol times, that is, step S140 will find the region maximum value of the noise characteristic change value between s = 83 and s = 123. Here, for convenience of explanation of the present embodiment, the time point corresponding to the maximum value of the region found in the i-th cycle is represented as T L (i).
然後,判斷此區域最大值所對應之時間點TL (i)是否落在時間點TG (i-1)前後一預設時間範圍內(例如時間點TG (i-1)前後10個符元時間內,也就是,s =93~s =113)(步驟S145)。Then, it is judged whether the time point T L (i) corresponding to the maximum value of the region falls within a preset time range before and after the time point T G (i-1) (for example, 10 times before and after the time point T G (i-1) In the symbol time, that is, s = 93 s = 113) (step S145).
若區域最大值所對應之時間點TL (i)落在時間點TG (i-1)前後的預設時間範圍內,則表示在觀察第i-1與第i週期後,雜訊的變化皆是落在時間點TG (i-1)前後的預設時間範圍內。因此,接下來,利用時間點TL (i)將週期分為第一時間區段與第二時間區段(步驟s150)。反之,若區域最大值所對應之時間點TL (i)並未落在時間點TG (i-1)前後的預設時間範圍內,則將不會切割週期(步驟S155),並回到步驟S105。If the time point T L (i) corresponding to the maximum value of the region falls within a preset time range before and after the time point T G (i-1), it means that after observing the i-1th and i th cycles, the noise is The changes are all within a preset time range before and after the time point T G (i-1). Therefore, next, the period is divided into the first time period and the second time period by using the time point T L (i) (step s150). On the other hand, if the time point T L (i) corresponding to the maximum value of the region does not fall within the preset time range before and after the time point T G (i-1), the cycle will not be cut (step S155), and Go to step S105.
舉例來說,在步驟S135中,每個符元所計算出之符元能量與雜訊特性變化值如圖4所示,而圖4(a)之縱座標為符元能量,圖4(b)之縱座標為雜訊特性變化值,圖4(c)之縱座標為雜訊型態索引,圖4之(a)、(b)、(c)之橫座標皆為符元時間索引。For example, in step S135, the symbol energy and the noise characteristic change value calculated by each symbol are as shown in FIG. 4, and the ordinate of FIG. 4(a) is the symbol energy, and FIG. 4(b) The ordinate of the symmetry is the change value of the noise characteristic. The ordinate of Fig. 4(c) is the noise type index, and the abscissas of (a), (b) and (c) of Fig. 4 are the symbol time index.
由圖4(b)可觀查出,在時間點TG (i-1)s =103的預設時間範圍內,存在有一區域最大值(剛好也出現於s =103之時間點),因此,在步驟S150中,利用s =103之時間點,將週期分為第一時間區段與第二時間區段。而圖4(c)中,第一時間區段為s =0~102,並對應雜訊型態索引為1。第二時間區段為s =103~199,並對應雜訊型態索引為2。It can be seen from Fig. 4(b) that there is a region maximum value (just at the time point of s = 103) within the preset time range of the time point T G (i-1) s = 103, therefore, In step S150, the period is divided into a first time period and a second time period using a time point of s = 103. In FIG. 4(c), the first time segment is s =0~102, and the corresponding noise type index is 1. The second time zone is s = 103~199, and the corresponding noise type index is 2.
請回頭參考圖1,在步驟S150之後,將更新符元紀錄表(步驟S157)。在更新符元紀錄表之後,符元紀錄表如圖5所示。圖5中,分別具有多個列欄位,來儲存每個時間區段之資料。而每個時間區段使用多個區塊來儲存其資料,而多個區塊分別為雜訊型態索引、起始時間、結束時間與下一時間區段。以第一時間區段為例,其資料儲存於符元紀錄表中的第一列欄位,其中,時間區段為1,雜訊型態索引為1,起始時間為s =0之時間點,結束時間為s =102之時間點,下一時間區段為時間區段為2(第二時間區段)。Referring back to FIG. 1, after step S150, the symbol record table will be updated (step S157). After updating the symbol record table, the symbol record table is shown in FIG. 5. In Figure 5, there are multiple column fields to store the data for each time segment. Each time segment uses multiple blocks to store its data, and the multiple blocks are the noise type index, start time, end time and next time segment. Taking the first time zone as an example, the data is stored in the first column of the symbol record table, wherein the time zone is 1, the noise type index is 1, and the start time is s =0. Point, the end time is the time point of s = 102, and the next time zone is the time zone of 2 (the second time zone).
值得一提的是,在圖5中之,利用一使用指標,來指示出週期內開始的時間區段,再利用一鏈接串列(link list)連接下一個時間區段,也就是,利用符元紀錄表中下一時間區的區塊,來指示出下一個時間區段。而圖5中,使用指標指向時間區段為1之區塊,而下一時間區段為2。另外,圖5中還利用一空閒指標,來指示出符元紀錄表中未使用的時間區段,並且同樣地利用一鏈接串列連接下一個未使用的時間區段。It is worth mentioning that, in FIG. 5, a usage indicator is used to indicate the time segment starting in the cycle, and then a link list is used to connect to the next time segment, that is, the use symbol. A block in the next time zone in the meta-record table to indicate the next time zone. In FIG. 5, the indicator is used to point to a block with a time segment of 1, and the next time segment is 2. In addition, an idle indicator is also utilized in FIG. 5 to indicate unused time segments in the symbol record table, and likewise to link the next unused time segment using a link string.
之後,重複步驟S105~S157,將能夠繼續依據雜訊的變化來分割週期,唯一不同的是,由於此時週期內已具有兩種雜訊型態(也就是雜訊型態索引為1與雜訊型態索引為2)。因此,在第i+1週期中,步驟S120中所利用的參考子頻帶雜訊能量noiseTemplate (b ),也會因雜訊型態分為兩 種參考子頻帶雜訊能量與兩種參考雜訊能量,也就是說,雜訊型態索引為1將對應24個不同子頻帶的參考子頻帶雜訊能量與1個參考雜訊能量。同樣地,雜訊型態索引為2將對應24個不同子頻帶的參考子頻帶雜訊能量與1個參考雜訊能量。After that, steps S105~S157 are repeated, and the cycle can be continued according to the change of the noise. The only difference is that there are two kinds of noise patterns in the cycle (that is, the noise type index is 1 and miscellaneous). The mode index is 2). Therefore, in the (i+1)th cycle, the reference sub-band noise energy noiseTemplate ( b ) used in step S120 is also divided into two kinds of reference sub-band noise energy and two kinds of reference noise energy due to the noise pattern. That is to say, the noise type index of 1 will correspond to the reference sub-band noise energy of 24 different sub-bands and one reference noise energy. Similarly, the noise type index of 2 will correspond to the reference sub-band noise energy of 24 different sub-bands and 1 reference noise energy.
因此,在步驟S120的子步驟S225中,則是利用符元紀錄表來找出此時的符元時間s 所在的時間區段,並找出所在的時間區段之雜訊型態索引,再利用此雜訊型態索引才能找出24個參考子頻帶雜訊能量,並以此24個參考子頻帶雜訊能量作為一參考值,來計算每個子頻帶能量差值。而在步驟S120的子步驟S255中,也將利用符元紀錄表來找出此時的符元時間s 所在的時間區段,並找出所在的時間區段之雜訊型態索引,才能依據雜訊型態索引來更新所對應的24個參考子頻帶雜訊能量。此外,在步驟S120的子步驟S260中,同樣地利用符元紀錄表來找出此時的符元時間s 所在的時間區段,並找出所在的時間區段之雜訊型態索引,才能依據雜訊型態索引來更新所對應的參考雜訊能量。Therefore, in sub-step S225 of step S120, the symbol record table is used to find the time segment in which the symbol time s is located at this time, and to find the noise type index of the time segment in which it is located, and then Using this noise type index, the 24 reference sub-band noise energy can be found, and the 24 reference sub-band noise energy is used as a reference value to calculate the energy difference of each sub-band. In the sub-step S255 of step S120, the symbol record table is also used to find the time segment where the symbol time s is located at this time, and the noise type index of the time segment in which the time zone is located can be found. The noise type index updates the corresponding 24 reference sub-band noise energy. In addition, in sub-step S260 of step S120, the symbol record table is similarly used to find the time zone in which the symbol time s is located at this time, and the noise type index of the time zone in which the time zone is located is found. The corresponding reference noise energy is updated according to the noise type index.
另外,在上述步驟中,雖然在第i-1週期是找出雜訊特性變化值中的全域最大值,並在第i週期是找出雜訊特性變化值中的區域最大值,並在i週期決定是否要分割週期。但是,本領域具通常知識者應當可以推知,依照上述的步驟,在每個週期內都可以同時地計算與尋找出全域最 大值與區域最大值,因此在每個週期內,皆可以依據全域最大值與區域最大值出現的時間點,來決定是否要分割週期。In addition, in the above step, although the global maximum value in the change value of the noise characteristic is found in the i-1th cycle, and the maximum value of the region in the change value of the noise characteristic is found in the i-th cycle, and The period determines whether or not to divide the period. However, those of ordinary skill in the art should be able to infer that, in accordance with the above steps, it is possible to simultaneously calculate and find the most global in each cycle. The large value and the maximum value of the region, so in each cycle, it is possible to decide whether to divide the cycle according to the time point at which the global maximum value and the regional maximum value appear.
另外,若在第i週期之後的第j-1週期中,找出一雜訊特性變化值的全域最大值,而其對應的時間點表示為TG (j-1)。並且,在第j週期中,找出時間點TG (j-1)前後一預設時間範圍內的區域最大值,而其對應的時間點表示為TL (j)(在此假設時間點TL (j)為s =136),則將時間點TL (i)與時間點TL (i)之間分割為第三時間區段。在分割出新的第三時間區段後,符元紀錄表將更新如圖6所示。由圖6可觀察出,新分割出來的第三時間區段位於符元紀錄表中的第三列欄位,並且具有一新的雜訊型態,對應至雜訊型態索引3。In addition, if in the j-1th cycle after the ith cycle, the global maximum value of a noise characteristic change value is found, and the corresponding time point is expressed as T G (j-1). And, in the jth cycle, the maximum value of the region within a predetermined time range before and after the time point T G (j-1) is found, and the corresponding time point is expressed as T L (j) (at this assumed time point) When T L (j) is s = 136), the time point T L (i) is separated from the time point T L (i) into a third time zone. After the new third time segment is segmented, the symbol record table will be updated as shown in FIG. 6. It can be observed from FIG. 6 that the newly segmented third time segment is located in the third column field in the symbol record table, and has a new noise pattern corresponding to the noise type index 3.
值得一提的是,雖然在上述的實施例中已經對依據雜訊特性分割週期的方法描繪出了一個可能的型態,但熟知此技術者應知,對於應用於各種通訊系統的方式都不一樣,因此本發明之應用當不限制於此種可能的型態。換言之,只要是在週期內找出一雜訊特性變化值中的最大值(在上述實施例中例如為區域最大值),在利用此最大值分割時間區段,就已經是符合了本發明的精神所在。It is worth mentioning that although in the above embodiments, a possible pattern has been drawn for the method of dividing the period according to the characteristics of the noise, those skilled in the art should know that the methods applied to various communication systems are not. Again, the application of the invention is therefore not limited to this possible type. In other words, as long as the maximum value of the noise characteristic change value is found in the period (for example, the region maximum value in the above embodiment), dividing the time segment by using the maximum value is already in accordance with the present invention. The spirit is there.
在上述實施例中,雖然將週期區分為第一、第二與第三時間區段,但本領域具通常知識者由上述實施例可知,本發明的精神在於依據雜訊特性來分割時間,因此本實施 例中之第一、第二與第三時間區段在實際的傳輸時間上並沒有一定的優先順序,僅是要表達出每個時間區段對應至一雜訊型態,並且,彼此之間的對應關係可以為多對一之對應關係。In the above embodiment, although the period is divided into the first, second, and third time segments, those skilled in the art can understand from the above embodiments that the spirit of the present invention is to divide the time according to the characteristics of the noise. This implementation The first, second and third time segments in the example do not have a certain priority in the actual transmission time, only to express each time segment corresponding to a noise pattern, and between each other The correspondence can be a many-to-one correspondence.
接下來,由於重複進行S105~S157,週期內將被切割為多個時間區段與多個雜訊型態。然而,在實際應用時,由於硬體上之限制(例如記憶體的容量等等),而使得週期內不能無限制的分割成過多的時間區段與過多的雜訊型態。因此,每當更新符元紀錄表後,將判斷所分割的時間區段的數量是否到達一第一設定值或雜訊型態數量是否到達一第二設定值(步驟S160)。其中,第一設定值為所分割之時間區段數量的最大值,第二設定值為雜訊型態數量的最大值。而第一設定值與第二設定值例如由收發端之設計者依據實際的硬體配置來決定,而本實施例中,假設第一設定值為8,而第二設定值為5。Next, since S105~S157 are repeated, the period will be cut into a plurality of time segments and a plurality of noise patterns. However, in practical applications, due to hardware limitations (such as the capacity of the memory, etc.), the period cannot be divided into excessive time segments and excessive noise patterns without limitation. Therefore, each time the symbol record table is updated, it is determined whether the number of divided time segments reaches a first set value or whether the number of noise patterns reaches a second set value (step S160). The first set value is a maximum value of the number of time segments divided, and the second set value is a maximum value of the number of noise patterns. The first set value and the second set value are determined, for example, by the designer of the transceiver end according to the actual hardware configuration. In this embodiment, the first set value is assumed to be 8 and the second set value is 5.
若步驟S160之判斷皆為否時,則回到步驟S105,繼續切割週期,若步驟S160之判斷其中之一為是時,將進行一合併步驟(步驟S170)。If the determination in step S160 is negative, the process returns to step S105 to continue the cutting cycle. If one of the determinations in step S160 is YES, a merge step is performed (step S170).
舉例來說,在第j週期之後的m-1週期中,每個符元所計算出之符元能量與雜訊特性變化值如圖7所示,而符元紀錄表被更新如圖8所示。由圖7與圖8可觀查出,時間區段之數量為6,雜訊型態的數量為5,由於雜訊型態的數量已到達第二設定值,因此將進行步驟S170。在本實施 例中,步驟S170包括多個子步驟,並繪示於圖9中。圖9繪示為步驟S170之子步驟的流程圖。For example, in the m-1 period after the jth period, the change of the symbol energy and the noise characteristic calculated by each symbol is as shown in FIG. 7, and the symbol record table is updated as shown in FIG. Show. As can be seen from FIG. 7 and FIG. 8, the number of time segments is 6, and the number of noise patterns is five. Since the number of noise patterns has reached the second set value, step S170 will be performed. In this implementation In the example, step S170 includes a plurality of sub-steps and is illustrated in FIG. FIG. 9 is a flow chart showing the sub-steps of step S170.
請參考圖9,開始依據雜訊型態合併時間週期(步驟S900)。首先,收發器在第m個週期接收傳輸通道中之符元(步驟S905)。在接下來的數個步驟(S910~S945)中,由於每個時間區段所進行之步驟皆相同,因此以圖7中之第四時間區段為例(其符元時間介於s =127~141),也就是圖8中的符元紀錄表內之時間區段為4之列欄位。Referring to FIG. 9, the time period is merged according to the noise pattern (step S900). First, the transceiver receives the symbols in the transmission channel at the mth cycle (step S905). In the next few steps (S910~S945), since the steps performed in each time segment are the same, the fourth time segment in FIG. 7 is taken as an example (the symbol time is between s =127). ~141), that is, the time zone in the symbol record table in Fig. 8 is a column of 4.
在步驟S910中,排除第四時間區段開始的暫態符元,其中暫態符元例如為每個時間區段開始的前面3個符元,也就是排除s =127,128,129時間點之符元。In step S910, the transient symbols starting from the fourth time segment are excluded, wherein the transient symbols are, for example, the first three symbols starting from each time segment, that is, the symbols excluding the s = 127, 128, 129 time points.
接下來,在第四時間區段中,計算一特定區段內之平均符元能量(步驟S915),其中,特定區段之長度例如為4個符元時間,也就是,利用圖2之步驟S235的計算方法來計算s =130,131,132,133,134時間點上符元能量後,再將4個符元能量其相加後除以4,以得到特定區段內之平均符元能量。Next, in the fourth time zone, the average symbol energy in a specific segment is calculated (step S915), wherein the length of the specific segment is, for example, 4 symbol times, that is, using the steps of FIG. The calculation method of S235 is to calculate the symbol energy at time points of s = 130, 131, 132, 133, 134, and then add the four symbol energies and divide them by 4 to obtain the average symbol energy in a specific segment.
在計算出第四時間區段之平均符元能量後,依據符元紀錄表,找出第四時間區段之前出現的雜訊型態(步驟S920)。而第四時間區段之起始時間為s =127,而在s =127之前的時間區段為第一至第二時間區段,而所對應的雜訊型態索引為1與2。After calculating the average symbol energy of the fourth time zone, the noise pattern appearing before the fourth time zone is found according to the symbol record table (step S920). The start time of the fourth time zone is s = 127, and the time zone before s = 127 is the first to second time zone, and the corresponding noise type indexes are 1 and 2.
接下來,利用所找出的雜訊型態,計算第四時間區段 對應每個雜訊型態之差值(步驟S925),其差值的計算方法為將步驟S915中所得到之平均符元能量與步驟S920中所找出之雜訊型態對應之參考雜訊能量noiseTempl atePower 相減,以得到對應每個雜訊型態之差值。之後,找出多個差值中的最小值,及其對應的雜訊型態索引(步驟S930),而其最小差值所對應的雜訊型態即為目標雜訊型態。Next, using the found noise pattern, calculating a difference between each of the noise patterns of the fourth time segment (step S925), the difference is calculated by using the average value obtained in step S915. The meta energy is subtracted from the reference noise energy noiseTempl at ePower corresponding to the noise pattern found in step S920 to obtain a difference corresponding to each of the noise patterns. Then, the minimum value of the plurality of differences and its corresponding noise type index are found (step S930), and the noise type corresponding to the minimum difference is the target noise type.
上述步驟S925與步驟S930中尋找最小值所對應之雜訊型態索引的計算方法如下所述:
上述y ,g 為一自然數,其中由於第一時間區段,其起始時間為s =0,因而在第一時間區段之前,沒有任何時間段,故上述之y 值介於2~6之間。The above y , g is a natural number, wherein the start time is s =0 due to the first time segment, so there is no time period before the first time segment, so the above y value is between 2 and 6 between.
接下來,在第四時間區段中,等待在特定區段(s =130~134)後的一延遲時間(步驟S935),並利用延遲時間之後的第一個符元,來計算其每個子頻帶的能量(步驟S940),而在本實施例中,假設此延遲時間為一符元時間,因此在第四時間區段中,延遲時間之後的第一個符元為s =135,而此符元中每個子頻帶的能量之計算方法如圖2中之步驟S220。Next, in the fourth time zone, waiting for a delay time after the specific zone ( s = 130~134) (step S935), and using the first symbol after the delay time to calculate each of its children The energy of the frequency band (step S940), and in the present embodiment, it is assumed that the delay time is one symbol time, so in the fourth time period, the first symbol after the delay time is s = 135, and this The calculation method of the energy of each sub-band in the symbol is as shown in step S220 in FIG.
之後,在第四時間區段中,利用延遲時間之後的第一個符元(s
=135之符元)中之每個子頻帶的能量,計算一合併距離(步驟S945)。合併距離的計算方法是利用在步驟S930中所找出的目標雜訊型態索引TargetTl,並利用類似於圖2中之步驟S230的計算方法,來得到第四時間區段的合併距離。其合併距離數學式如下所述:
接下來,假設執行步驟S910~S945以得到每個時間區段所對應的合併距離,因此,在下一個步驟中,將找出最小的合併距離mergeDist (s ),及其對應之時間區段(步驟S950)。並將具有最小的合併距離mergeDist (s )之時間區段的雜訊型態索引設定為目標雜訊型態索引TargetTl(步驟S955),也就是,將具有最小的合併距離mergeDist (s )之時間區段所對應的的雜訊型態索引合併至目標雜訊型態索引 TargetTl。Next, it is assumed that steps S910 to S945 are performed to obtain the merge distance corresponding to each time segment, and therefore, in the next step, the smallest merge distance mergeDist ( s ), and its corresponding time segment will be found (step S950). And setting the noise type index of the time segment having the smallest merge distance mergeDist ( s ) to the target noise type index TargetT1 (step S955), that is, the time having the smallest merge distance mergeDist ( s ) The noise type index corresponding to the segment is merged into the target noise type index TargetTl.
在本實施例中,假設找出第六時間區段(也就是圖8中之時間區段為6之列欄位)具有最小的合併距離mergeDist (s ),而其目標雜訊型態索引TargetTl例如為3,因此,將第六時間區段的雜訊型態索引設置為3。In this embodiment, it is assumed that the sixth time zone (that is, the time zone of the time zone of FIG. 8 is 6) has the smallest merge distance mergeDist ( s ), and its target noise type index TargetTl. For example, it is 3, therefore, the noise type index of the sixth time zone is set to 3.
在最後一個步驟中,將更新符元紀錄表(步驟S960),並如圖10所示。而由圖10與圖8之差別只在於,第六時間區段(也就是時間區段為6之列欄位)所對應之雜訊型態索引由5轉變為3。而將第五時間區段的雜訊型態合併至目標雜訊型態索引TargetTl後,如圖11所示。由於在合併步驟S170中,並未計算雜訊特性變化值,因此,圖11(b)中空白。由圖11(c)可觀查出,第五時間區段對應的雜訊型態索引設置為3。In the last step, the symbol record table will be updated (step S960) and as shown in FIG. The difference between FIG. 10 and FIG. 8 is only that the noise type index corresponding to the sixth time segment (that is, the time segment is 6 columns) is changed from 5 to 3. After the noise pattern of the fifth time segment is merged into the target noise type index TargetTl, as shown in FIG. Since the noise characteristic change value is not calculated in the merging step S170, the blank in Fig. 11(b) is blank. It can be seen from FIG. 11(c) that the noise type index corresponding to the fifth time zone is set to 3.
接下來,在更新符元紀錄表後,將回到圖1中之步驟S160,繼續判斷所分割的時間區段的數量是否到達一第一設定值或雜訊型態數量是否到達一第二設定值時。Next, after updating the symbol record table, it will return to step S160 in FIG. 1 to continue to determine whether the number of divided time segments reaches a first set value or whether the number of noise patterns reaches a second setting. When the value is.
若步驟S160之判斷皆為否時,則回到圖1之步驟S105,繼續切割週期,若步驟S965之判斷其中之一為是時,則回到步驟S170,繼續合併雜訊型態或時間區段。If the determination in step S160 is negative, then return to step S105 of FIG. 1 to continue the cutting cycle. If one of the determinations of step S965 is YES, then return to step S170 to continue to merge the noise pattern or time zone. segment.
綜上所述,本發明透過偵測雜訊能量的變化以及雜訊在頻譜上之變化,將一週期分割為多個時間區段,並且讓每個時間區段對應到一雜訊之型態,以讓收發端能夠得知此時雜訊的型態。因此,收發端能夠依據此時的雜訊型態, 適當地調整例如傳輸之位元率或傳輸信號之能量大小。In summary, the present invention divides a period into a plurality of time segments by detecting changes in noise energy and changes in noise in the spectrum, and causes each time segment to correspond to a noise pattern. So that the transceiver can know the type of noise at this time. Therefore, the transceiver can be based on the noise pattern at this time. The bit rate of the transmission or the amount of energy of the transmitted signal is appropriately adjusted.
雖然本發明已以較佳實施例揭露如上,然其並非用以限定本發明,任何熟習此技藝者,在不脫離本發明之精神和範圍內,當可作些許之更動與潤飾,因此本發明之保護範圍當視後附之申請專利範圍所界定者為準。While the present invention has been described in its preferred embodiments, the present invention is not intended to limit the invention, and the present invention may be modified and modified without departing from the spirit and scope of the invention. The scope of protection is subject to the definition of the scope of the patent application.
S100~S170‧‧‧本發明實施例之依據雜訊型態分割週期的方法之各步驟S100~S170‧‧‧ steps of the method according to the embodiment of the invention according to the noise pattern segmentation period
S210~260‧‧‧步驟S120之子步驟Substeps of S210~260‧‧‧Step S120
S900~960‧‧‧步驟S170之子步驟Sub-steps of S900~960‧‧‧Step S170
圖1繪示為本發明實施例之依據雜訊型態分割週期的方法步驟流程圖。FIG. 1 is a flow chart showing the steps of a method according to a noise pattern segmentation cycle according to an embodiment of the present invention.
圖2繪示為步驟S120之子步驟的流程圖。FIG. 2 is a flow chart showing the sub-steps of step S120.
圖3(a)繪示為每個符元所對應之符元能量。Figure 3 (a) shows the symbol energy corresponding to each symbol.
圖3(b)繪示為每個符元所對應之雜訊特性變化值。FIG. 3(b) illustrates the change in the noise characteristic corresponding to each symbol.
圖3(c)繪示為週期內之時間分割及對應的雜訊型態索引。Figure 3 (c) shows the time division in the period and the corresponding noise pattern index.
圖4(a)繪示為每個符元所對應之符元能量。Figure 4 (a) shows the symbol energy corresponding to each symbol.
圖4(b)繪示為每個符元所對應之雜訊特性變化值。Figure 4(b) shows the change in the noise characteristic corresponding to each symbol.
圖4(c)繪示為週期內之時間分割及對應的雜訊型態索引。Figure 4(c) shows the time division in the period and the corresponding noise pattern index.
圖5繪示為符元紀錄表。Figure 5 is a symbol record table.
圖6繪示為符元紀錄表。Figure 6 is a symbol record table.
圖7(a)繪示為每個符元所對應之符元能量。Figure 7 (a) shows the symbol energy corresponding to each symbol.
圖7(b)繪示為每個符元所對應之雜訊特性變化值。FIG. 7(b) shows the variation value of the noise characteristic corresponding to each symbol.
圖7(c)繪示為週期內之時間分割及對應的雜訊型態索引。Figure 7(c) shows the time division in the period and the corresponding noise pattern index.
圖8繪示為符元紀錄表。Figure 8 is a symbol record table.
圖9繪示為步驟S170之子步驟的流程圖。FIG. 9 is a flow chart showing the sub-steps of step S170.
圖10繪示為符元紀錄表。Figure 10 is a symbol record table.
圖11(a)繪示為每個符元所對應之符元能量。Figure 11 (a) shows the symbol energy corresponding to each symbol.
圖11(b)繪示為每個符元所對應之雜訊特性變化值。Figure 11 (b) shows the change in the noise characteristic corresponding to each symbol.
圖11(c)繪示為週期內之時間分割及對應的雜訊型態索引。Figure 11 (c) shows the time division within the period and the corresponding noise pattern index.
S100~S170‧‧‧本發明實施例之依據雜訊型態分割週期的方法之各步驟S100~S170‧‧‧ steps of the method according to the embodiment of the invention according to the noise pattern segmentation period
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