CN103180751A - Arrival angle calculation device - Google Patents
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- CN103180751A CN103180751A CN2011800519041A CN201180051904A CN103180751A CN 103180751 A CN103180751 A CN 103180751A CN 2011800519041 A CN2011800519041 A CN 2011800519041A CN 201180051904 A CN201180051904 A CN 201180051904A CN 103180751 A CN103180751 A CN 103180751A
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Abstract
Description
技术领域technical field
本发明涉及检测到达的电波的相位而用于电波到达角度的计算的到达角度计算装置。The present invention relates to an arrival angle calculating device which detects the phase of an arriving radio wave and uses it for calculating the arrival angle of the radio wave.
背景技术Background technique
在以往的到达方向估计装置中,使用互相关系数的计算、逆矩阵运算等运算量大的运算,需要几百符号量的运算。因此,希望得到可以通过简便的运算来估计到达方向的到达方向估计装置。In the conventional direction-of-arrival estimating apparatus, calculations requiring a large amount of calculations, such as calculations of cross-correlation coefficients and inverse matrix calculations, require calculations of hundreds of symbols. Therefore, it is desired to obtain a direction-of-arrival estimating device that can estimate the direction of arrival through simple calculations.
在专利文献1中提出了缩小了运算规模的到达方向估计装置。在专利文献1所记载的到达方向估计装置中,对由两个天线接收到的接收信号,由复共轭电路和乘法电路来计算到达方向的系数,通过在到达方向检测电路中进行反正切运算和反余弦运算,而估计了接收波的到达方向。
现有技术文献prior art literature
专利文献patent documents
专利文献1:日本特开平10-177064号公报Patent Document 1: Japanese Patent Application Laid-Open No. 10-177064
发明内容Contents of the invention
发明要解决的课题The problem to be solved by the invention
但是,在专利文献1中,采用了比较1隙缝间的到达方向矢量的功率与阈值、并在比阈值大的情况下更新到达方向的构成,因此,有可能不能够准确地检测接收波中的期望波来更新到达方向。例如,在接收波的背景值高的情况下,与期望波的信号电平无关地,接收波的功率往往比阈值大。在这种情况下,在背景值下到达方向也被计算、更新,因此不能够正确估计到达方向。However, in
本发明是鉴于这样的点而进行的,其目的在于提供一种可以抑制接收波的背景值的影响、并能够以高精度计算到达角度的到达角度计算装置。The present invention has been made in view of such points, and an object of the present invention is to provide an arrival angle calculation device capable of suppressing the influence of background values of received waves and calculating an arrival angle with high precision.
用于解决课题的手段means to solve the problem
本发明的到达角度计算装置的特征在于,具备:多个天线,接收从某个位置发送的电波;多个接收信号处理部,与所述各天线对应地设置;以及到达角度计算部,从由所述多个接收信号处理部输出的输出信号取入在接收信号处理部间成为相同信息单位的信号分量从而计算所述电波的到达角度,所述各接收信号处理部具备:接收部,将由对应的所述天线接收到的电波变换为具有该电波的相位信息的接收信号并输出;相关处理部,将从所述接收部输出的接收信号进行相关处理;峰值检测部,检测进行了所述相关处理的接收信号的峰值;以及定时控制部,以从所述相关处理部的输出信号切出在所述接收信号处理部间成为相同信息单位的信号分量的方式,与由所述峰值检测部检测到的峰值的定时相配合,从而控制从所述相关处理部输出的输出信号的取入定时,在与所述信息单位相当的期间中的峰值期间的电力与除了该峰值期间以外的期间的电力之比大于阈值的情况下,所述定时控制部将来自所述相关处理部的信号向所述到达角度计算部输出。The angle of arrival calculation device of the present invention is characterized in that it includes: a plurality of antennas for receiving radio waves transmitted from a certain position; a plurality of received signal processing units provided corresponding to the antennas; and an angle of arrival calculation unit configured from The output signals outputted by the plurality of received signal processing units take in signal components that are the same information unit among the received signal processing units to calculate the angle of arrival of the radio waves, and each of the received signal processing units includes: a receiving unit configured by a corresponding The electric wave received by the antenna is converted into a received signal having phase information of the electric wave and output; the correlation processing unit performs correlation processing on the received signal output from the receiving unit; the peak detection unit detects that the correlation has been performed. a peak value of the received signal to be processed; and a timing control unit that is detected by the peak detection unit in such a manner that a signal component that becomes the same information unit between the received signal processing units is cut out from the output signal of the correlation processing unit. In accordance with the timing of the peak value, the timing of taking in the output signal output from the correlation processing unit is controlled, and the power during the peak period and the power during the period other than the peak period in the period corresponding to the information unit are controlled. When the ratio is larger than the threshold value, the timing control unit outputs the signal from the correlation processing unit to the angle-of-arrival calculation unit.
根据该构成,将峰值期间的电力和其以外的期间的电力之比与阈值相比较,在比大于阈值的情况下计算到达角度,因此即使在接收波的期望波以外的信号电平高的情况下,也可以准确地检测期望波的峰值,并计算到达角度。即,没有根据期望波以外的部分计算到达角度,因此可以提高到达角度的计算精度。According to this configuration, the ratio between the power during the peak period and the power during other periods is compared with the threshold value, and when the ratio is greater than the threshold value, the angle of arrival is calculated. Therefore, even when the signal level of the received wave other than the desired wave is high Under this condition, it is also possible to accurately detect the peak of the desired wave and calculate the angle of arrival. That is, since the angle of arrival is not calculated from parts other than the desired wave, the calculation accuracy of the angle of arrival can be improved.
在本发明的到达角度计算装置中,也可以为,将∑P1和∑P2之比∑P1/∑P2与阈值进行比较,在所述比∑P1/∑P2大于所述阈值的情况下,所述定时控制部将来自所述相关处理部的信号向所述到达角度计算部输出,其中上述∑P1是与所述信息单位相当的期间中的峰值期间的电力之和,上述∑P2是与所述信息单位相当的期间中除了所述峰值期间以外的期间中的电力之和。In the angle of arrival calculation device of the present invention, it is also possible to compare the ratio ΣP 1 /ΣP 2 between ΣP 1 and ΣP 2 with a threshold value, and when the ratio ΣP 1 /ΣP 2 is greater than the In the case of a threshold value, the timing control unit outputs the signal from the correlation processing unit to the angle-of-arrival calculation unit, wherein the above-mentioned ΣP 1 is the sum of the electric power during the peak period in the period corresponding to the information unit , the above-mentioned ΣP 2 is the sum of electric power in periods other than the peak period in the period corresponding to the information unit.
在本发明的到达角度计算装置中,也可以为,所述到达角度计算部具备:复共轭部,取来自一方的接收信号处理部的定时控制部的信号的复共轭,该一方的接收信号处理部与一方的天线对应;复数乘法部,将所述复共轭部的输出和来自另一方的接收信号处理部的定时控制部的信号相乘,该另一方的接收信号处理部与另一方的天线对应;反正切部,使用所述复数乘法部的输出来进行反正切运算,计算所述天线间的所述接收电波的相位差;平均化部,对所述反正切部的输出进行平均化;以及到达角度变换部,使用所述平均化部的输出来进行反三角函数运算,从而变换为到达角度。根据该构成,可以不使用互相关系数的计算、逆矩阵运算等而计算到达角度,因此可以缩小到达角度计算装置的规模。In the angle-of-arrival calculation device of the present invention, the angle-of-arrival calculation unit may include: a complex conjugate unit that takes the complex conjugate of the signal from the timing control unit of one reception signal processing unit, and the one reception signal processing unit The signal processing part corresponds to one antenna; the complex multiplication part multiplies the output of the complex conjugate part and the signal from the timing control part of the other received signal processing part, and the received signal processing part of the other party is connected to the other antenna. one antenna corresponds; the arctangent part uses the output of the complex multiplication part to perform an arctangent calculation, and calculates the phase difference of the received radio wave between the antennas; the averaging part performs an arctangent calculation on the output of the arctangent part Averaging; and an arrival angle conversion unit that performs an inverse trigonometric calculation using the output of the averaging unit to convert it into an arrival angle. According to this configuration, the angle of arrival can be calculated without using the calculation of the correlation coefficient, the inverse matrix operation, and the like, so that the scale of the angle-of-arrival calculation device can be reduced.
在本发明的到达角度计算装置中,也可以为,在计算出的所述相位差分布在I-Q平面上的+180°及/或-180°附近的情况下,所述到达角度计算部在使各相位差旋转规定角度后进行平均化,从该平均值减去所述规定角度后进行反三角函数运算,从而变换为到达角度。根据该构成,在相位差分布在到达角度的计算精度处于降低的倾向的相位差区域的情况下,使相位差仅旋转规定角度而进行到达角度计算的运算,因此到达角度的计算精度才没有降低。结果,可以充分提高到达角度的计算精度。In the angle-of-arrival calculation device of the present invention, the angle-of-arrival calculation unit may use each The phase difference is averaged after being rotated by a predetermined angle, the predetermined angle is subtracted from the average value, and an inverse trigonometric function is performed to convert it into an arrival angle. According to this configuration, when the phase difference is distributed in the phase difference region where the calculation accuracy of the angle of arrival tends to decrease, the calculation of the angle of arrival is performed by rotating the phase difference by only a predetermined angle, so that the calculation accuracy of the angle of arrival does not decrease. . As a result, the calculation accuracy of the angle of arrival can be sufficiently improved.
在本发明的到达角度计算装置中,也可以为,在所述I-Q平面上,在大于+90°或小于-90°的相位差的数量比小于+90°且大于-90°的相位差的数量多的情况下,判断为分布在所述I-Q平面上的+180°及/或-180°附近。In the angle of arrival calculation device of the present invention, on the I-Q plane, the number of phase differences greater than +90° or less than -90° may be greater than the number of phase differences less than +90° and greater than -90° In the case of , it is determined that they are distributed in the vicinity of +180° and/or -180° on the I-Q plane.
在本发明的到达角度计算装置中,也可以为,使所述规定角度为+90°、-90°、+180°或-180°的任一个角度。In the arrival angle calculation device of the present invention, the predetermined angle may be any angle of +90°, -90°, +180°, or -180°.
在本发明的到达角度计算装置中,也可以为,在所述复数乘法部的输出的I分量为负、且所述复数乘法部的输出的I分量的绝对值与Q分量的绝对值相比充分大的情况下,通过在反转了所述Q分量的符号后进行调换了I分量与Q分量的关系的反正切运算,来计算校正后的相位差,对所述校正后的相位差进行平均化,从该平均值减去90°后进行反三角函数运算,从而变换为到达角度。根据该构成,在相位差分布在到达角度的计算精度处于降低的倾向的相位差区域的情况下,使相位差旋转规定角度的量而进行到达角度计算的运算,因此到达角度的计算精度才没有降低。结果,可以充分提高到达角度的计算精度。In the angle of arrival calculation device of the present invention, the I component of the output of the complex multiplication unit may be negative, and the absolute value of the I component of the output of the complex multiplication unit may be compared with the absolute value of the Q component. If it is sufficiently large, the corrected phase difference is calculated by performing an arctangent operation in which the relationship between the I component and the Q component is reversed after the sign of the Q component is reversed, and the corrected phase difference is calculated. After averaging, 90° is subtracted from the average value, and an inverse trigonometric function operation is performed to convert it into an angle of arrival. According to this configuration, when the phase difference distribution is in the phase difference region where the calculation accuracy of the angle of arrival tends to decrease, the calculation of the angle of arrival is performed by rotating the phase difference by a predetermined angle, so that the calculation accuracy of the angle of arrival is not high. reduce. As a result, the calculation accuracy of the angle of arrival can be sufficiently improved.
在本发明的到达角度计算装置中,也可以为,在所述复数乘法部的输出的I分量为负、且所述复数乘法部的输出的I分量的绝对值与Q分量的绝对值相比充分大的情况下,通过在反转了所述I分量的符号后进行调换了I分量与Q分量的关系的反正切运算,来计算校正后的相位差,对所述校正后的相位差进行平均化,对该平均值加上90°后进行反三角函数运算,从而变换为到达角度。根据该构成,在相位差分布在到达角度的计算精度处于降低的倾向的相位差区域的情况下,使相位差旋转规定角度的量而进行到达角度计算的运算,因此到达角度的计算精度才没有降低。结果,可以充分提高到达角度的计算精度。In the angle of arrival calculation device of the present invention, the I component of the output of the complex multiplication unit may be negative, and the absolute value of the I component of the output of the complex multiplication unit may be compared with the absolute value of the Q component. If it is sufficiently large, the corrected phase difference is calculated by performing an arctangent operation in which the relationship between the I component and the Q component is reversed after the sign of the I component is reversed, and the corrected phase difference is calculated. For averaging, add 90° to the average value and perform an inverse trigonometric function operation to convert it into an arrival angle. According to this configuration, when the phase difference distribution is in the phase difference region where the calculation accuracy of the angle of arrival tends to decrease, the calculation of the angle of arrival is performed by rotating the phase difference by a predetermined angle, so that the calculation accuracy of the angle of arrival is not high. reduce. As a result, the calculation accuracy of the angle of arrival can be sufficiently improved.
在本发明的到达角度计算装置中,也可以为,在所述复数乘法部的输出的I分量为负、且所述复数乘法部的输出的I分量的绝对值与Q分量的绝对值相比充分大的情况下,通过在反转了所述I分量的符号和Q分量的符号后进行反正切运算来计算校正后的相位差,对所述校正后的相位差进行平均化,从该平均值减去180°后进行反三角函数运算,从而变换为到达角度。根据该构成,在相位差分布在到达角度的计算精度处于降低的倾向的相位差区域的情况下,使相位差旋转规定角度的量而进行到达角度计算的运算,因此到达角度的计算精度才没有降低。结果,可以充分提高到达角度的计算精度。In the angle of arrival calculation device of the present invention, the I component of the output of the complex multiplication unit may be negative, and the absolute value of the I component of the output of the complex multiplication unit may be compared with the absolute value of the Q component. If it is sufficiently large, the corrected phase difference is calculated by performing an arctangent operation after inverting the sign of the I component and the Q component, the corrected phase difference is averaged, and from the average After the value is subtracted by 180°, the inverse trigonometric function operation is performed to transform it into the arrival angle. According to this configuration, when the phase difference distribution is in the phase difference region where the calculation accuracy of the angle of arrival tends to decrease, the calculation of the angle of arrival is performed by rotating the phase difference by a predetermined angle, so that the calculation accuracy of the angle of arrival is not high. reduce. As a result, the calculation accuracy of the angle of arrival can be sufficiently improved.
发明效果Invention effect
根据本发明的到达角度计算装置,求出峰值期间的电力与峰值期间以外的剩余的期间中的电力的比,对该求出的比和阈值进行比较,在比大于阈值的情况下计算到达角度,因此即使在接收波的期望波以外的信号电平高的情况下,也可以准确地检测期望波的峰值,并计算到达角度。即,没有根据期望波以外的部分计算到达角度,因此可以提高到达角度的计算精度。According to the angle-of-arrival calculating device of the present invention, the ratio of the electric power during the peak period to the electric power during the remaining periods other than the peak period is obtained, the obtained ratio is compared with a threshold value, and the angle of arrival is calculated when the ratio is larger than the threshold value. , so even when the signal level of the received wave other than the desired wave is high, the peak of the desired wave can be accurately detected and the angle of arrival can be calculated. That is, since the angle of arrival is not calculated from parts other than the desired wave, the calculation accuracy of the angle of arrival can be improved.
附图说明Description of drawings
图1是表示实施方式涉及的到达角度计算装置的构成例的框图。FIG. 1 is a block diagram showing a configuration example of an arrival angle calculation device according to the embodiment.
图2是表示实施方式涉及的到达角度计算装置的具体的构成(DSSS)的框图。FIG. 2 is a block diagram showing a specific configuration (DSSS) of the angle-of-arrival calculation device according to the embodiment.
图3是表示加法器的输出波形的例的图。FIG. 3 is a diagram showing an example of an output waveform of an adder.
图4(a)是表示反正切部的输出波形的例的图,(b)是表示电力计算部的输出波形的例的图。FIG. 4( a ) is a diagram showing an example of an output waveform of an arctangent unit, and FIG. 4( b ) is a diagram showing an example of an output waveform of an electric power calculation unit.
图5是表示到达天线的电波的几何学关系的示意图。Fig. 5 is a schematic diagram showing the geometric relationship of radio waves reaching the antenna.
图6是表示包括到达角度计算装置的位置检测系统的例的示意图。FIG. 6 is a schematic diagram showing an example of a position detection system including an arrival angle calculation device.
图7是到达角度计算装置中的到达角度计算的流程图。Fig. 7 is a flow chart of the angle of arrival calculation in the angle of arrival calculation device.
图8是向峰值检测部输入的信号的示意图。FIG. 8 is a schematic diagram of signals input to a peak detection unit.
图9是表示作为调制方式而使用DSSS的情况下向峰值检测部输入的信号的例的示意图。FIG. 9 is a schematic diagram showing an example of a signal input to a peak detection unit when DSSS is used as a modulation scheme.
图10是表示向使用AD变换器而取入了接收信号的情况下的峰值检测部输入的信号的例的示意图。FIG. 10 is a schematic diagram showing an example of a signal input to a peak detection unit when a received signal is acquired using an AD converter.
图11是表示到达角度计算部的其它例的框图。FIG. 11 is a block diagram showing another example of an arrival angle calculation unit.
图12是表示相位差的计算范围的示意图。FIG. 12 is a schematic diagram showing a calculation range of a phase difference.
图13是表示计算的相位差数据的例的示意图。FIG. 13 is a schematic diagram showing an example of calculated phase difference data.
图14是表示相位差成为+180°或-180°附近的情况下的到达角度计算的概略的示意图。FIG. 14 is a schematic diagram showing an outline of angle-of-arrival calculation when the phase difference is in the vicinity of +180° or −180°.
图15是相位差成为+180°或-180°附近的情况下的到达角度计算的流程图。FIG. 15 is a flowchart of angle-of-arrival calculation when the phase difference is in the vicinity of +180° or −180°.
图16是表示到达角度计算部的其它例的框图。FIG. 16 is a block diagram showing another example of an arrival angle calculation unit.
图17是表示实施方式涉及的到达角度计算装置的具体的构成(OFDM)的框图。FIG. 17 is a block diagram showing a specific configuration (OFDM) of the angle-of-arrival calculation device according to the embodiment.
图18(a)是表示OFDM中的符号的构成的示意图,(b)是表示OFDM符号串的相关处理的情况的示意图。FIG. 18( a ) is a schematic diagram showing a symbol configuration in OFDM, and FIG. 18( b ) is a schematic diagram showing a state of correlation processing of OFDM symbol strings.
图19(a)(b)是表示来自电力计算部的输出波形的例的图,(c)是表示来自加法部的输出波形的例的图,(d)是表示来自反正切部的各部分的输出波形的例的图。19 (a) and (b) are diagrams showing examples of output waveforms from the power calculation unit, (c) are diagrams showing examples of output waveforms from the addition unit, and (d) are diagrams showing each part from the arctangent unit A diagram of an example of the output waveform.
图20是表示使用了到达角度计算装置的胶囊内窥镜系统的构成例的示意图。FIG. 20 is a schematic diagram showing a configuration example of a capsule endoscope system using an arrival angle calculation device.
具体实施方式Detailed ways
图1是表示本发明的一实施方式涉及的到达角度计算装置的构成例的框图。本实施方式涉及的到达角度计算装置1具备:基准信号发生部10,能够以规定的振荡频率振荡基准信号;接收用天线11a、11b,隔开规定间隔地配置;接收部12a、12b,使用从基准信号发生部10输出的基准信号而将由接收用天线11a、11b接受的电波变换为接收信号并输出;以及运算部13,根据从接收部12a、12b输出的接收信号来进行用于到达角度计算的各种运算处理。另外,到达角度计算装置1,根据由电波的传播延迟引起的相位滞后来计算到达角度,因此需要在隔开规定间隔的二个点(或二个以上的点)接收具有相同的信息的电波。因此,需要具备与接收电波对应的两个(或其以上)的天线及接收系统。另外,只要可以在隔开规定间隔的二个以上的位置接收相同的到达电波(相同的信息单位),到达角度计算装置1并不限定于具备二个以上的接收系统的构成。FIG. 1 is a block diagram showing a configuration example of an arrival angle calculation device according to an embodiment of the present invention. The angle-of-
接收部12a、12b构成为包括低噪声放大器、混频器、带通滤波器等,并构成为能够接收规定频率的电波。运算部13构成为包括:相关处理部21a、21b,进行接收信号的相关处理;峰值检测部22a、22b,检测进行了相关处理的接收信号的峰值;定时控制部23a、23b,配合由峰值检测部22a、22b检测到的峰值的定时而输出来自相关处理部21a、21b的信号;以及到达角度计算部24,根据来自定时控制部23a、23b的信号,来进行到达角度的计算。另外,运算部13的构成、功能可以由硬件实现,也可以由软件实现。The receiving
相关处理部21a、21b将来自接收部12a、12b的接收信号和与该接收信号相关高的信号相乘并输出。在相关处理部21a、21b中被乘的信号与接收信号的相关高,因此从相关处理部21a、21b输出的信号在相关区间成为峰值。峰值检测部22a、22b计算来自相关处理部21a、21b的输出信号的电力,并检测输出信号的电力峰值。定时控制部23a、23b配合在峰值检测部22a、22b中检测到的峰值定时,而将来自相关处理部21a、21b的输出信号向到达角度计算部24输出。具体地,基于根据所检测的峰值期间的电力而计算的信息,来决定是否将来自相关处理部21a、21b的输出信号向到达角度计算部24输出。The
图2表示作为调制方式而使用直接频谱扩展(DSSS)的情况下的到达角度计算装置的具体的构成例的框图。另外,在图2中仅表示了与图1中的运算部13相当的构成。FIG. 2 is a block diagram showing a specific configuration example of an angle-of-arrival calculation device when direct spectrum spread (DSSS) is used as a modulation scheme. In addition, in FIG. 2, only the structure corresponding to the
在图2中,相关处理部21a具备:发生扩散码的扩散码发生器31;将接收信号和扩散码相乘的乘法器32a及32b;以及将乘法器32a及32b的输出合计1位(bit)期间量并向峰值检测部22a及定时控制部23a输出的加法器33a及33b。峰值检测部22a具备:计算从加法器33a及33b输出的信号的电力的电力计算部34a;以及检测其电力峰值并向定时控制部23a输出的峰值电力检测部35a。定时控制部23a具备缓存部36a,基于来自峰值电力检测部35a的信号来控制来自加法器33a及33b的信号可否向到达角度计算部24输出。同样,相关处理部21b具备扩散码发生器31、乘法器32c及32d、加法器33c及33d,峰值检测部22b具备电力计算部34b、峰值电力检测部35b,定时控制部23b具备缓存部36b。到达角度计算部24具备:取缓存部36a的输出的复共轭的复共轭部41;将复共轭部41的输出和缓存部36b的输出复数相乘的复数乘法部42;使用复数乘法部42的输出来进行反正切运算的反正切部43;根据复数乘法部42的输出信号来计算每个码片(chip)区间的电力的电力计算部44;根据来自电力计算部44的信息将反正切部43的输出平均化的平均化部45;以及使用平均化部45的输出来变换为到达角度的到达角度变换部46。In FIG. 2 , the
扩散码发生器31发生用于将通过DSSS扩展到频率轴上的信号解扩的扩散码。该扩散码与在发送侧码调制(扩展)时使用的扩散码对应。乘法器32a及32b将接收信号乘上上述扩散码而进行解扩。向乘法器32a输入来自接收部12a的接收信号中的同相分量I1。此外,向乘法器32b输入来自接收部12a的接收信号中的正交分量Q1。加法器33a及33b在与1位相当的期间(位区间)内相加乘法器32a及32b的每个码片区间的输出并输出。图3(a)表示来自加法器33a的输出波形的例。图3(b)是图3(a)所示的输出波形的部分放大图。此外,图3(c)表示来自加法器33b的输出波形的例。图3(d)是图3(c)所示的输出波形的部分放大图。The spreading
将加法器33a的输出信号及加法器33b的输出信号向峰值检测部22a的电力计算部34a及定时控制部23a的缓存部36a输入。电力计算部34a根据加法器33a及33b的输出信号来计算每个码片区间的电力。具体地,电力计算部34a将与同相分量相当的加法器33a的输出信号的绝对值和与正交分量相当的加法器33b的输出信号的绝对值相加,作为每个码片区间的电力信息而向峰值电力检测部35a输出。峰值电力检测部35a,当接受每个码片区间的电力信息时,检测接收信号中的电力峰值,作为电力峰值信息而向定时控制部23a的缓存部36a输出。另外,也可以将加法器33a的输出信号的平方值和加法器33b的输出信号的平方值相加而向峰值电力检测部35a输出。The output signal of the
从峰值检测部22a(峰值电力检测部35a)输出的电力峰值信息为,判定接收信号的峰值的有无的信息。具体地,电力峰值信息为,表示接收信号的峰值点附近的期间(峰值期间)内的电力之和∑P1与从成为DSSS中的信息单位的1位期间除去了峰值期间以外的期间中的电力之和∑P2的比R(=∑P1/∑P2)是否大于阈值Rth的信息。在电力峰值信息中,在R大于Rth的情况下,定时控制部23a(缓存部36a)认为在该定时接收信号具有峰值,而将1位量的信号Ia1及信号Qa1向到达角度计算部24输出。另一方面,在R小于Rth的情况下,定时控制部23a(缓存部36a)认为在该定时接收信号不具有峰值,而停止向到达角度计算部24的输出。另外,此处,峰值检测部22a进行了与电力峰值信息有关的运算处理,但也可以在定时控制部23a中进行与电力峰值信息有关的运算处理。The power peak information output from the
相关处理部21b(扩散码发生器31、乘法器32c及32d、加法器33c及33d)、峰值检测部22b(电力计算部34b、峰值电力检测部35b)、定时控制部23b(缓存部36b)的动作、功能,与上述相关处理部21a(扩散码发生器31、乘法器32a及32b、加法器33a及33b)、峰值检测部22a(电力计算部34a、峰值电力检测部35a)、定时控制部23a(缓存部36a)的动作、功能同样。只是,向相关处理部21b输入的接收信号与向相关处理部21a输入的接收信号,由于在隔开规定间隔的二点接收相同电波,因此相位稍微不同。因此,从定时控制部23b输出的信号与从定时控制部23a输出的信号的相位稍微不同。当将与同相分量相当的信号作为实部、将与正交分量相当的信号作为虚部而由复数来表现定时控制部23a的输出Oa1、及定时控制部23b的输出Oa2时,成为下述式(1)、(2)那样。另外,及表示各信号的相位。
【式1】【Formula 1】
【式2】[Formula 2]
定时控制部23a的输出Oa1被输入到达角度计算部24的复共轭部41。复共轭部41将定时控制部23a的输出Oa1的复共轭向复数乘法部42输出。即,从复共轭部41输出信号Ia1和将信号Qa1的符号反转了的信号。当用复数表示复共轭部41的输出Oa1′时,成为下述式(3)那样。The output O a1 of the
【式3】[Formula 3]
复数乘法部42将复共轭部41的输出Oa1′与定时控制部23b的输出Oa2复数相乘,并将作为相乘结果的信号Ib及信号Qb向反正切部43及电力计算部44输出。复数乘法部42的输出Ob、输出Ob的同相分量Ib及正交分量Qb表示为如下述式(4)~(6)那样。The
【式4】[Formula 4]
【式5】[Formula 5]
Ib=Ia1×Ia2+Qa1×Qa2 …(5)Ib=Ia1×Ia2+Qa1×Qa2 ...(5)
【式6】[Formula 6]
Qb=Qa1×Ia2-Ia1×Qa2 …(6)Qb=Qa1×Ia2-Ia1×Qa2 ...(6)
反正切部43使用复数乘法部42的输出来进行反正切运算。具体地,进行以复数乘法部42的输出信号Ib为分母、以输出信号Qb为分子的值的反正切运算。图4(a)表示来自反正切部43的输出波形的例。反正切部43的输出Oarctan与相位差相当,由下述式(7)表示。The
【式7】[Formula 7]
电力计算部44根据复数乘法部42的输出信号来计算每个码片区间的电力。具体地,电力计算部44将Ib的绝对值和Qb的绝对值相加,并作为每个码片区间的电力信息而向平均化部45输出。另外,也可以将Ib的平方值和Qb的平方值相加而向平均化部45输出。图4(b)表示来自电力计算部44的输出波形的例。平均化部45,当接受每个码片区间的电力信息时,根据该信息来将反正切部43的输出Oarctan平均化而向到达角度变换部46输出。另外,电力计算部44及平均化部45也可以适当省略。The
到达角度变换部46使用平均化部45的输出(在不具有平均化部45的情况下,使用反正切部43的输出)并通过反三角函数运算来变换为到达角度。作为反三角函数运算,例如,可以应用反正弦运算。由该运算求出的值、即到达角度变换部46的输出与到达角度θ(rad)相当。到达角度变换部46的输出Oarcsin由下述式(8)表示。另外,在下述式中,λ(m)为接收波的波长,d(m)为接收用天线间的距离。The arrival
【式8】[Formula 8]
由上述处理得到到达角度,是由于图5所示那样的几何学关系成立。设到达以规定的方向为基准而隔开间隔d(m)配置的两个接收用天线11a、11b的电波所成的角度为θ(rad)。到达接收用天线11b的电波的传播距离,与到达接收用天线11a的电波的传播距离相比长Δ(m),产生相位延迟(相位差(rad))。当用接收波的波长λ(m)来表示在该模型中产生的传播距离的差分Δ与相位差的关系时,成为下述式(9)那样。另外,在下述式中,Δ<λ。The reason for obtaining the angle of arrival by the above processing is that the geometric relationship shown in FIG. 5 is established. The angle formed by the radio waves arriving at the two receiving
【式9】[Formula 9]
此外,根据上述模型中的传播距离的差分Δ、天线间隔d、到达角度θ的几何学关系,下述式(10)成立。In addition, the following formula (10) holds true from the geometric relationship of the propagation distance difference Δ, the antenna spacing d, and the arrival angle θ in the above model.
【式10】[Formula 10]
Δ=dsinθ …(10)Δ=dsinθ ...(10)
即,到达角度θ就会表示为下述式(11)那样。另外,式(11)与到达角度变换部46中的处理相当。这样可知,能够由本实施方式的到达角度计算装置来计算到达角度。That is, the angle of arrival θ is expressed as in the following equation (11). In addition, Expression (11) corresponds to the processing in the arrival
【式11】[Formula 11]
接着,对使用了到达角度计算装置的位置检测系统的例进行说明。图6所示的位置检测系统101构成为包括到达角度计算装置1a、与到达角度计算装置1a隔开规定距离D而配置的其它到达角度计算装置1b、接入点2或用户终端3。接入点2及用户终端3构成为,分别具备发送系统及接收系统(未图示),能够进行双向的信息传输(通信)。此外,接入点2及用户终端3构成为,可以通过各自具备的发送系统而向到达角度计算装置1a及到达角度计算装置1b发送到达角度计算用的电波。位置检测的对象为接入点2或用户终端3的任一个均可。Next, an example of a position detection system using an arrival angle calculation device will be described. The
到达角度计算装置1a通过接收用天线11aa及11ab来接收从接入点2的发送用天线发送的电波,从而计算以到达角度计算装置1a为基准的到达角度。此外,到达角度计算装置1b通过接收用天线11ba及11bb来接收从接入点2的发送用天线发送的电波,从而计算以到达角度计算装置1b为基准的到达角度。如果到达角度计算装置1a和到达角度计算装置1b的位置关系已知,则可以根据以各自为基准的到达角度来决定接入点2的位置。The angle-of-arrival calculation device 1a receives radio waves transmitted from the transmission antenna of the
此外,在用户终端3的位置检测的情况下,到达角度计算装置1a及到达角度计算装置1b计算从用户终端3发送的电波的到达角度。In addition, in the case of detecting the position of the user terminal 3 , the angle-of-arrival calculation device 1 a and the angle-of-arrival calculation device 1 b calculate the angle of arrival of radio waves transmitted from the user terminal 3 .
图7是本实施方式涉及的到达角度计算装置1中的到达角度计算的流程图。当到达角度计算装置1接收到达角度计算对象的电波时,接收部12a、12b向相关处理部21a、21b输出接收信号。此后,相关处理部21a、21b在步骤201中进行接收信号的相关处理及加法处理。FIG. 7 is a flowchart of the angle-of-arrival calculation in the angle-of-
此后,峰值检测部22a、22b在步骤202中根据相关处理部21a、21b的输出信号来检测电力的峰值Ppeak。此后,计算峰值点附近的期间(峰值期间)内的电力之和∑P1与从1位期间(信息单位的期间)除去了峰值期间以外的期间中的电力之和∑P2,并计算它们的比R(=∑P1/∑P2)。图8(a)示意地表示向峰值检测部22a、22b输入的信号。峰值电力Ppeak为图8(a)中的峰值点P上的电力,∑P1为峰值期间t1中的电力之和,∑P2为从1位期间除去了峰值期间t1的期间t2中的电力之和。此处,峰值期间t1为包括峰值的升降区间的期间。例如,如图9所示,在作为调制方式而使用DSSS的情况下,能够形成扩散码的周期tc的2倍的升降区间。因此,可以设该2·tc的期间为峰值期间t1。另外,在图9中,期间t2使用1位期间tb而表示为tb-2·tc。Thereafter, in
图10表示向使用AD变换器而取入了接收信号的情况下的峰值检测部22a、22b输入的信号的例。图10的横轴t表示样本编码,t取离散的值。在作为调制方式而使用DSSS的情况下,例如,如果扩散码为11码片、1位期间为1μs,则扩散码的1码片期间为0.091μs。如果设AD变换为1码片期间的4倍的过采样,则升降区间扩展1码片量,成为ips=ip-3、ipe=ip+3。在这种情况下,R表示为下述式(12)那样。FIG. 10 shows an example of signals input to the
【数12】【Number 12】
在步骤203中,峰值检测部22a、22b将所计算的比R(=∑P1/∑P2)与规定的阈值Rth相比较。在R比Rth大的情况下,峰值检测部22a、22b将该内容的信号向定时控制部23a、23b输出。定时控制部23a,当接受R比Rth大的内容的信号时,认为接收信号存在峰值,而将到达角度的计算所需的信号向到达角度计算部24输出。此后,在步骤204中,到达角度计算部24计算到达角度。另一方面,在R为Rth以下的情况下,峰值检测部22a、22b将该内容的信号向定时控制部23a、23b输出,定时控制部23a,认为接收信号不存在峰值,而停止向到达角度计算部24的输出。此后,到达角度计算装置1再次执行从步骤201开始的流程。Rth为任意的值。例如,可以将通过与R的比较来判定峰值的有无的程度的值设定为Rth。In
这样,通过将与所检测的峰值有关的指标(R)与阈值(Rth)相比较来判定峰值的有无,能够准确地判定峰值的有无。In this way, by comparing the index (R) related to the detected peak value with the threshold value (R th ) to determine the presence or absence of the peak value, it is possible to accurately determine the presence or absence of the peak value.
此处,单纯对将功率(电力)与功率的阈值相比较来判定峰值的有无的方法进行考察。图8(b)示意地表示背景值高的信号(实线)和背景值低的信号(虚线)。在图8(b)中,在如虚线所示那样背景值低的情况下,可以通过将功率的峰值与功率的阈值Pth相比较,来检测峰值。但是,在图8(b)中,当如实线所示那样背景值高到超过Pth的程度时,即使将功率的峰值与Pth相比较也不能够检测峰值。这是因为,在功率的峰值与功率的阈值的单纯的比较中,不能考虑背景值。所以,如本实施方式所示那样,通过在峰值的检测中使用考虑了背景值的指标,可以准确地判定峰值的有无。Here, a method of simply comparing power (electric power) with a threshold value of power to determine the presence or absence of a peak will be considered. Figure 8(b) schematically represents a signal with a high background value (solid line) and a signal with a low background value (dashed line). In FIG. 8( b ), when the background value is low as indicated by the dotted line, the peak value can be detected by comparing the peak value of the power with the threshold value P th of the power. However, in FIG. 8( b ), when the background value is high enough to exceed P th as indicated by the solid line, the peak value cannot be detected even if the peak value of the power is compared with P th . This is because the background value cannot be considered in a simple comparison of the peak value of the power and the threshold value of the power. Therefore, as shown in the present embodiment, by using an index that takes the background value into consideration for detection of a peak, the presence or absence of a peak can be accurately determined.
如以上所示那样,本实施方式涉及的到达角度计算装置,通过求出峰值期间的电力与峰值期间以外的剩余的期间中的电力的比、并比较该求出的比与阈值来判定峰值的有无,即使在接收波的背景值高的情况下也可以准确地检测期望波的峰值并用于到达角度的计算。即,没有根据期望波以外的信号分量来计算到达角度,因此可以提高到达角度的计算精度。As described above, the angle of arrival calculation device according to this embodiment determines the peak value by calculating the ratio of the power during the peak period to the power in the remaining periods other than the peak period, and comparing the calculated ratio with a threshold value. With or without, even when the background value of the received wave is high, the peak of the desired wave can be accurately detected and used for the calculation of the angle of arrival. That is, since the angle of arrival is not calculated from signal components other than the desired wave, the calculation accuracy of the angle of arrival can be improved.
图11是说明到达角度计算装置1中的到达角度计算部24的另一形态的框图。图11所示的到达角度计算部24具备:取定时控制部23a的输出Oa1的复共轭的复共轭部51;将复共轭部51的输出Oa1′与定时控制部23b的输出Oa2复数相乘的复数乘法部52;以及使用复数乘法部52的输出来进行反正切运算的反正切部53。复共轭部51、复数乘法部52、反正切部53的动作、功能,与上述的复共轭部41、复数乘法部42、反正切部43的动作、功能同样。此外具备:基于反正切部53的运算结果(相位差)来校正运算结果的相位差校正部54;将相位差校正部54的输出平均化的平均化部55;在相位差校正部54中进行了校正的情况下校正平均化部55的运算结果(平均值)的相位差再校正部56;以及使用相位差再校正部56的输出而变换为到达角度的到达角度变换部57。到达角度变换部57的动作、功能,与上述的到达角度变换部46的动作、功能同样。FIG. 11 is a block diagram illustrating another form of the arrival
相位差校正部54,在作为反正切部53的运算结果的相位差成为+180°(+π)附近、-180°(-π)附近的值的情况下,进行在反正切部的运算结果中加上规定的角度(相位差)的处理。如图12的I-Q平面所示,本实施方式的到达角度计算部24将相位差投影到-180°~+180°(-π~+π)的相位差范围的坐标上。因此,例如,如图13(a)所示,在由反正切部53计算的相位差不成为+180°及-180°附近的值的情况下,通过将其平均化,而可以适当地计算到达角度。但是,如图13(b)所示,在由反正切部53计算的相位差成为+180及-180附近的值的情况下,所计算的相位差的少许误差就会对角度计算施加大的影响。此处,假定为作为相位差数据而得到-178°及+178°的两个值,作为一方的值的+178°是基于作为本来的值的-178°产生-4°的误差后而成为+178°的。它们的差实际上仅为4°。但是,在平均化处理中,当作为-178°和+178°而平均化时,平均值成为0°。尽管实际上存在约180°的相位差,但通过平均化处理会作为0°来处理。这样,当所平均化的相位差从本来的相位差大幅度偏离时,适当的到达角度计算变得困难。The phase
所以,图11所示的到达角度计算部24,在由反正切部53计算的相位差成为+180°及-180°附近的值的情况下,相位差校正部54进行在反正切部53的运算结果中加上规定的角度(相位差)的校正处理,而进行适当的平均化。反正切部53的运算结果是否为+180°或-180°附近的值,可以基于作为反正切部53的运算结果而得到的多个相位差的分布来判定。例如,在大于+90°(+π/2)或小于-90°(-π/2)的相位差的数量、比小于+90°并且大于-90°的相位差的数量多的情况下,可以判定为反正切部53的运算结果为+180°及-180°附近的值。可以使相位差校正部54所加上的角度(相位差)例如为+90°,但只要是能够进行适当的平均化处理的角度,并非限定于此。优选地,也可以为-90°、+180°或-180°的任一个。Therefore, in the angle-of-
平均化部55将相位差校正部54的输出平均化。本实施方式的到达角度计算部24,在计算不适于平均化的相位差的情况下进行加上相位差的校正,因此能够在平均化部55中进行适当的平均化处理。相位差再校正部56,在相位差校正部54中进行了相位差的校正的情况下,校正平均化部55的输出。具体地,进行减去在相位差校正部54中作为校正值而加上了的角度(相位差)的校正。The averaging
图14示意地表示相位差成为+180°及-180°附近的情况下的到达角度计算的概略。在由反正切部53计算的相位差在I-Q平面中为+180°及-180°附近的情况下,相位差校正部54在相位差中加上校正值(+90°)而使坐标轴旋转,并变换为平均值计算用的坐标轴。平均化部55基于该数据来计算平均值(-92°)。相位差再校正部56进行从相位差校正部54的输出数据减去校正值(+90°)的校正,并向反正弦部57输出所校正后的数据(+178°)。FIG. 14 schematically shows the outline of calculation of the angle of arrival when the phase difference is in the vicinity of +180° and −180°. When the phase difference calculated by the
图15是上述到达角度计算部24中的处理流程图。到达角度计算部24的复共轭部51在步骤301中计算定时控制部23a的输出Oa1的复共轭。此外,复数乘法部52在步骤302中将定时控制部23b的输出Oa2和复共轭部51的输出Oa1′相乘。此后,反正切部53在步骤303中使用复数乘法部52的输出来进行反正切运算,计算接收信号间的相位差。FIG. 15 is a flowchart of processing in the above-mentioned angle-of-
在步骤304中,相位差校正部54判定所计算的相位差在I-Q平面中是否为+180°及-180°附近的值。在所计算的相位差并非+180°及-180°附近的值的情况下,进入步骤305,到达角度计算部24不校正相位差而计算到达角度。在所计算的相位差为+180°附近或-180°附近的值的情况下,进入步骤306。该判定,如上述那样,可以以大于+90°或小于-90°的相位差的数量是否比小于+90°并且大于-90°的相位差的数量多为基准来进行。In
在步骤306中,相位差校正部54进行在作为反正切部53的运算结果的相位差中加上90°的处理。在步骤307中,平均化部55将相位差校正部54的输出平均化。此后,在步骤308中,相位差再校正部56进行从作为平均化部55的运算结果的平均值减去90°的处理。此后,在步骤309中,到达角度变换部57根据相位差再校正部56的输出来计算到达角度。这样,在图11所示的到达角度计算部24中,通过在加上规定的相位差并平均化之后减去规定的相位差的一系列的处理而计算适当的平均值,因此到达角度的计算精度才没有降低。结果,可以充分提高到达角度的计算精度。In
另外,此处,相位差校正部54进行在反正切部53的运算结果中加上规定的角度的处理,但只要可以实现适当的平均化处理,并非限定于此。例如,也可以使用图16所示那样的构成的到达角度计算部24。图16所示的到达角度计算部24具备:取定时控制部23a的输出Oa1的复共轭的复共轭部61;以及将复共轭部61的输出Oa1′与定时控制部23b的输出Oa2复数相乘的复数乘法部62。复共轭部61、复数乘法部62的动作、功能,与上述的复共轭部41、复数乘法部42的动作、功能同样。此外具备:将复数乘法部62的输出的同相分量(I分量)的绝对值与正交分量(Q分量)的绝对值相比较的IQ比较部63;以及使用复数乘法部62的输出,根据IQ比较部63的输出来选择、变更运算方法,而进行反正切运算的反正切部64。此外具备:将作为反正切部64的运算结果的相位差平均化的平均化部65;根据反正切部64的运算方法来校正作为平均化部65的运算结果的平均值的相位差再校正部66;以及使用相位差再校正部66的输出而变换为到达角度的到达角度变换部67。到达角度变换部67的动作、功能,与上述的到达角度变换部46的动作、功能同样。In addition, here, the phase
IQ比较部63判定复数乘法部的输出的同相分量(I分量)是否为负,并且比较复数乘法部62的输出的同相分量(I分量)的绝对值与正交分量(Q分量)的绝对值。具体地,IQ比较部63判定同相分量Ib的符号,并且判定同相分量的绝对值︱Ib︱与正交分量的绝对值︱Qb︱相比是否充分大(正交分量的绝对值︱Qb︱与同相分量的绝对值︱Ib︱相比是否充分小)。在接收信号的相位差在I-Q平面中取+180°及-180°附近的值的情况下,同相分量Ib为负(Ib<0),同相分量的绝对值︱Ib︱与正交分量的绝对值︱Qb︱相比充分大。因此,通过判定同相分量Ib的符号、并判定同相分量的绝对值︱Ib︱与正交分量的绝对值︱Qb︱相比是否充分大,可以判定相位差是否取+180°及-180°附近的值。The
反正切部64使用复数乘法部62的输出,根据IQ比较部63的输出来选择运算方法而进行反正切运算。在同相分量为正的情况下、同相分量为负并且同相分量的绝对值︱Ib︱与正交分量的绝对值︱Qb︱为相同程度或比其小的情况下,进行以复数乘法部62的输出Ib为分母、以输出Qb为分子的值的反正切运算。在同相分量为负并且同相分量的绝对值︱Ib︱与正交分量的绝对值︱Qb︱相比充分大的情况下,例如,进行以使复数乘法部62的输出Qb的符号反转了的-Qb为分母、以输出Ib为分子的值的反正切运算。另外,在同相分量的绝对值︱Ib︱与正交分量的绝对值︱Qb︱相比充分大的情况下的上述处理,与使坐标轴旋转+90°而进行反正切运算的处理相当。即,由该处理得到的相位差为在原来的相位差中加上了+90°的值。The
另外,在同相分量的绝对值︱Ib︱与正交分量的绝对值︱Qb︱相比充分大的情况下的处理,并非限定于上述的处理。例如,也可以进行以复数乘法部62的输出Qb为分母、以使输出Ib的符号反转了的-Ib为分子的值的反正切运算。该处理,与使坐标轴旋转-90°而进行反正切运算的处理相当。即,由该处理得到的相位差为在原来的相位差中加上了-90°的值(减去了+90°的值)。此外,例如也可以使复数乘法部62的输出Ib的符号和输出Qb的符号反转而进行反正切运算。该处理,与使坐标轴旋转+180°(或-180°)而进行反正切运算的处理相当。即,由该处理得到的相位差为在原来的相位差中加上了+180°(或-180°)的值。通过这种处理,也可以计算适当的平均值。In addition, the processing when the absolute value |Ib| of the in-phase component is sufficiently larger than the absolute value |Qb| of the quadrature component is not limited to the above-mentioned processing. For example, an arctangent calculation may be performed using the output Qb of the
平均化部65将反正切部64的输出平均化。本实施方式的到达角度计算部24在计算不适于平均化的相位差的情况下进行实质上加上(或减去)相位差的校正,因此能够在平均化部65中进行适当的平均化处理。相位差再校正部66在反正切部64进行了使坐标轴旋转+90°的处理的情况下,校正平均化部65的输出。具体地,进行减去+90°的校正。另外,在反正切部64进行了使坐标轴旋转-90°的处理的情况下,进行减去-90°的校正(即加上+90°的校正)。同样,在反正切部64进行了使坐标轴旋转+180°(或-180°)的处理的情况下,进行减去+180°(或-180°)的校正。The averaging
这样,图16所示的到达角度计算部24也可以与图11所示的到达角度计算部24同样地计算适当的平均值,因此到达角度的计算精度才没有降低。结果,可以充分提高到达角度的计算精度。In this way, the arrival
图17是表示作为调制方式而使用正交频分复用(OFDM)的情况下的到达角度计算装置的具体的构成例的框图。另外,在图17中,仅示出了与图1中的运算部13相当的构成。FIG. 17 is a block diagram showing a specific configuration example of an angle-of-arrival calculation device when orthogonal frequency division multiplexing (OFDM) is used as a modulation scheme. In addition, in FIG. 17, only the structure corresponding to the
在图17中,相关处理部21a具备:取接收部12a的输出的复共轭的复共轭部71a;使接收部12a的输出延迟规定期间的量并输出的延迟部72a;将复共轭部71a的输出和延迟部72a的输出复数相乘的复数乘法部73a;以及仅在GI(保护间隔)期间相加复数乘法部73a的输出并输出的加法器74a、74b。峰值检测部22a具备:计算从加法器74a、74b输出的信号的电力的电力计算部75a;以及检测其电力峰值并向定时控制部23a输出的峰值电力检测部76a。定时控制部23a具备基于来自峰值电力检测部76a的信号来控制来自接收部12a的信号向到达角度计算部24的输出定时的延迟部77a。同样,相关处理部21b具备复共轭部71b、延迟部72b、复数乘法部73b、加法器74c、74d,峰值检测部22b具备电力计算部75b、峰值电力检测部76b,定时控制部23b具备延迟部77b。到达角度计算部24具备:取延迟部77a的输出的复共轭的复共轭部81;将复共轭部81的输出和延迟部77b的输出复数相乘的复数乘法部82;仅在GI(保护间隔)期间相加复数乘法部42的输出并输出的加法部83a、83b;使用加法部83a、83b的输出来进行反正切运算的反正切部84;将反正切部84的输出平均化的平均化部85;以及使用平均化部85的输出来变换为到达角度的到达角度变换部86。In FIG. 17 , the
延迟部72a、72b取OFDM符号串的自相关,因此使接收部12a的输出延迟规定期间的量并输出。具体地,延迟部72a、72b,为了将复共轭部71a输出的OFDM符号的尾部与延迟部72a、72b输出的GI(保护间隔)在相同的定时向复数乘法部73a输入,而使接收部12a的输出延迟规定期间的量并输出。复数乘法部73a将复共轭部71a的输出和延迟部72a的输出复数相乘。加法器74a及74b仅在GI期间相加复数乘法部73a的每个码片区间的输出并输出。The
图18(a)是表示OFDM符号串的构成的示意图。如图18(a)所示,OFDM符号串由作为数据部的OFDM符号和配置在OFDM符号的起始的GI构成。GI为拷贝了OFDM符号尾部的数据,为了防止OFDM符号间的干扰而被插入。图18(b)是表示相关处理部21a中的OFDM符号串的相关处理(自相关处理)的情况的示意图。如图18(a)所示,延迟部72a的输出相对复共轭部71a的输出延迟了OFDM符号长度的量。因此,在复数乘法部73a中,可以通过复共轭部71a的输出和延迟部72a的输出相乘而取自相关。自相关值(GI相关值)在复共轭部71a的输出和延迟部72a的输出中出现与GI相同的数据时示出峰值,因此通过使用这一点,而可以检测作为数据部的OFDM符号的起始。FIG. 18( a ) is a schematic diagram showing the structure of an OFDM symbol sequence. As shown in FIG. 18( a ), an OFDM symbol sequence is composed of an OFDM symbol as a data part and a GI arranged at the head of the OFDM symbol. The GI copies the data at the end of the OFDM symbol and is inserted to prevent interference between OFDM symbols. FIG. 18( b ) is a schematic diagram showing a state of correlation processing (autocorrelation processing) of OFDM symbol sequences in the
加法器74a及74b的输出信号被输入峰值检测部22a的电力计算部75a。电力计算部75a根据加法器74a及74b的输出信号来计算每个码片区间的电力。具体地,电力计算部34a将与同相分量相当的输出信号的绝对值和与正交分量相当的输出信号的绝对值相加,作为每个码片区间的电力信息而向峰值电力检测部76a输出。另外,也可以将与同相分量相当的输出信号的平方值和与正交分量相当的输出信号的平方值相加并向峰值电力检测部76a输出。图19(a)表示来自电力计算部75a的输出波形的例。图19(b)是图19(a)所示的输出波形的部分放大图。峰值电力检测部76a当接受每个码片区间的电力信息时,检测接收信号中的电力峰值,作为电力峰值信息而向定时控制部23a的延迟部77a输出。The output signals of the
从峰值检测部22a(峰值电力检测部35a)输出的电力峰值信息为判定接收信号的峰值的有无的信息。具体地,电力峰值信息为,表示接收信号的峰值点附近的期间(峰值期间)内的电力之和∑P1与从成为OFDM中的信息单位的1符号期间除去了峰值期间以外的期间中的电力之和∑P2的比R(=∑P1/∑P2)是否大于阈值Rth大的信息。在作为调制方式而使用OFDM的情况下,峰值期间与GI期间相等。此外,所谓1符号期间,与合计了GI期间和数据期间(OFDM符号期间)的期间相当。在电力峰值信息中,在R大于Rth的情况下,定时控制部23a(延迟部77a)认为在该定时接收信号具有峰值,而将来自接收部12a的接收信号向到达角度计算部24。另一方面,在R小于Rth的情况下,定时控制部23a(延迟部77a)认为在该定时接收信号不具有峰值,而停止向到达角度计算部24的输出。另外,此处,峰值检测部22a进行了与电力峰值信息有关的运算处理,但也可以在定时控制部23a中进行与电力峰值信息有关的运算处理。The power peak information output from the
相关处理部21b(复共轭部71b、延迟部72b、复数乘法部73b、加法器74c、74d)、峰值检测部22b(电力计算部75b、峰值电力检测部76b)、定时控制部23b(延迟部77b)的动作、功能,与相关处理部21a(复共轭部71a、延迟部72a、复数乘法部73a、加法器74a、74b)、峰值检测部22a(电力计算部75a、峰值电力检测部76a)、定时控制部23a(延迟部77a)的动作、功能同样。只是,向相关处理部21b输入的接收信号和向相关处理部21a输入的接收信号,由于在隔开规定间隔的二点接收了相同电波,因此相位稍微不同。因此,在从定时控制部23b输出的信号与从定时控制部23a输出的信号中,相位稍微不同。
定时控制部23a的输出被输入到达角度计算部24的复共轭部81。复共轭部81将定时控制部23a的输出的复共轭向复数乘法部82输出。复数乘法部82将复共轭部81的输出和定时控制部23b的输出复数相乘,并将运算结果向加法部83a及83b输出。加法部83a及83b在GI期间相加复数乘法部82的每个码片区间的输出并向反正切部84输出。图19(c)表示来自加法部83a及83b的输出波形的例。在图中,加法部83a的输出波形由I表示,加法部83b的输出波形由Q表示。The output of the
反正切部84使用加法部83a及83b的输出来进行反正切运算,计算接收信号的相位差。图19(d)表示来自反正切部84的输出波形的例。平均化部85将反正切部84的输出平均化并向到达角度变换部86输出。另外,平均化部85也可以适当省略。到达角度变换部86使用平均化部85的输出(在不具有平均化部85的情况下,反正切部84的输出)并通过反三角函数运算来变换为到达角度。由该运算求出的值、即到达角度变换部86的输出与到达角度相当。The
这样,在具有图17的运算部13的到达角度计算装置1中,也通过求出峰值期间的电力与峰值期间以外的剩余的期间中的电力的比、并比较该求出的比与阈值来判定峰值的有无,即使在接收波的背景值高的情况下也可以准确地检测期望波的峰值并用于到达角度的计算。即,没有根据期望波以外的信号分量来计算到达角度,因此可以提高到达角度的计算精度。In this way, also in the angle-of-
图20是表示将到达角度计算装置1应用于胶囊内窥镜的位置特定的胶囊内窥镜系统的示意图。图20所示的胶囊内窥镜系统具备多个传感器阵列401、记录来自传感器阵列401的数据的数据记录器402。传感器阵列401具备与到达角度计算装置1的接收用天线相当的天线,并构成为可以接收来自患者吞下的胶囊内窥镜的电波。数据记录器402根据传感器阵列401中接收到的电波具有的相位信息,来确定患者吞下的胶囊内窥镜的位置。FIG. 20 is a schematic diagram showing a position-specific capsule endoscope system in which the angle-of-
患者吞下的胶囊内窥镜通过消化道的蠕动运动而移动。胶囊内窥镜的位置被监视,可以确认是否到达了诊察部位。当胶囊内窥镜到达诊察部位时,胶囊内窥镜将诊察部位的情况摄影并向数据记录器402发送,数据记录器402记录图像信息。这样,通过监视胶囊内窥镜的位置,而可以不看漏诊察部位而进行摄影。此外,能够在胶囊内窥镜到达了诊察部位的定时接通照相机等的电源,并在脱离了诊察部位的情况下切断照相机等的电源,因此可以减小电池容量。此外,能够削减传感器(天线)的数量。此外,如果电池容量相同,与以往类型的胶囊内窥镜相比较可以发送大量的图像,可以得到鲜明的图像。The endoscope capsule, swallowed by the patient, is moved by the peristaltic motion of the digestive tract. The position of the capsule endoscope is monitored, and it can be confirmed whether it has reached the examination site. When the capsule endoscope arrives at the examination site, the capsule endoscope takes pictures of the examination site and sends them to the
这样,通过将到达角度计算装置1应用于胶囊内窥镜的位置确定,可以构筑优良的胶囊内窥镜系统。In this way, by applying the angle-of-
如以上那样,根据本发明的到达角度计算装置,求出峰值期间的电力与峰值期间以外的剩余的期间中的电力的比,并比较该求出的比和阈值,在比大于阈值的情况下计算到达角度,因此即使在接收波的期望波以外的信号电平高的情况下,也可以准确地检测期望波的峰值,并计算到达角度。即,没有根据期望波以外的部分计算到达角度,因此可以提高到达角度的计算精度。As described above, according to the angle-of-arrival calculation device of the present invention, the ratio of the electric power during the peak period to the electric power during the remaining periods other than the peak period is obtained, and the obtained ratio is compared with the threshold value. If the ratio is greater than the threshold value, The angle of arrival is calculated, so even when the signal level of the received wave other than the desired wave is high, the peak of the desired wave can be accurately detected and the angle of arrival can be calculated. That is, since the angle of arrival is not calculated from parts other than the desired wave, the calculation accuracy of the angle of arrival can be improved.
另外,本发明并非限定于上述实施方式的记载,可以以发挥其效果的方式适当变更。例如,在上述实施方式中,将峰值期间的电力之和与除了峰值期间以外的期间的电力之和的比、与阈值相比较,但只要能够进行考虑了期望波以外的信号的电平的到达角度计算,并不限定于此。例如,也可以使用峰值期间的某个定时的电力和除了峰值期间以外的期间的某个定时的电力作为参数。In addition, this invention is not limited to description of said embodiment, It can change suitably so that the effect may be exhibited. For example, in the above-mentioned embodiment, the ratio of the sum of the electric power during the peak period to the sum of the electric power during periods other than the peak period is compared with the threshold, but as long as the arrival of the level of the signal other than the desired wave can be considered Angle calculation is not limited to this. For example, power at a certain timing during the peak period and power at a certain timing during periods other than the peak period may be used as parameters.
此外,在上述实施方式中,附图所示的构成等并非限定于此,能够在发挥本发明的效果的范围内适当变更。In addition, in the said embodiment, the structure etc. which are shown in drawing are not limited to this, It can change suitably within the range which exhibits the effect of this invention.
产业上的可利用性Industrial availability
本发明的到达角度计算装置可以用于确定对象的位置的系统、及其它各种用途。The angle-of-arrival calculation device of the present invention can be used in a system for specifying the position of an object, and in various other applications.
本申请是基于2010年11月12日提出的日本特愿2010-254011号,并包含了其全部内容。This application is based on Japanese Patent Application No. 2010-254011 filed on November 12, 2010 and incorporates the entire content thereof.
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| WO2012063532A1 (en) | 2012-05-18 |
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