首页>
外国专利>
METHOD AND SYSTEM FOR RECOVERY signals in the form of periodically repeating pulses (PPI) with rapidly tunable deconvolution METHOD AND THEIR USE
METHOD AND SYSTEM FOR RECOVERY signals in the form of periodically repeating pulses (PPI) with rapidly tunable deconvolution METHOD AND THEIR USE
展开▼
机译:用快速可调的反卷积恢复周期性重复脉冲(PPI)形式的信号的方法和系统及其应用
展开▼
页面导航
摘要
著录项
相似文献
摘要
1.method u0432u043eu0441u0441u0442u0430u043du043eu0432u043bu0435u043du0438u00a0 u0434u0438u0441u043au0440u0435u0442u0438u0437u0438u0440u043eu0432u0430u043du043du043eu0433u043e signal x (tm) in the form of a periodically u043fu043eu0432u0442u043eu0440u00a0u044eu0449u0438u0445u0441u00a0 pulses with fast frequency that can be set by u0434u0435u043au043eu043du0432u043eu043bu044eu0446u0438u0438, opinion u044eu0447u0430u044eu0449u0438u0439u0441u00a0 that pulses with the same frequency of u043eu0431u044au0435u0434u0438u043du00a0u044eu0442 between a packet (u0441u0442u0430u0434u0438u00a0 S0)the transforming from the time domain into the frequency signals (u0441u0442u0430u0434u0438u00a0 s2) and the spectra are u0434u0435u043au043eu043du0432u043eu043bu044eu0446u0438u0438 (u0441u0442u0430u0434u0438u00a0 claims).;2. method for 1, in which the conversion from the time domain to the frequency (u0441u0442u0430u0434u0438u00a0 s2) u0432u044bu043fu043eu043bu043du00a0u044eu0442 also u0432u044bu0447u0438u0441u043bu0435u043du0438u00a0 by discrete fourier u0438u043cu043fu0443u043bu044cu0441u043e u043fu0440u0435u043eu0431u0440u0430u0437u043eu0432u0430u043du0438u00a0 in u043eu0442u0441u0447u0435u0442u043eu0432 frequency.;3. method for 1, in which the conversion from the time domain to the frequency (u0441u0442u0430u0434u0438u00a0 s2) u0432u044bu0447u0438u0441u043bu00a0u044eu0442 also u043eu043fu0440u0435u0434u0435u043bu00a0u0435u043cu044bu0439 sampling method of dft (c) and u043du0430u0445u043eu0434u00a0u0442 knowl u0447u0435u043du0438u00a0 his l different from u043du0443u043bu00a0 u0441u043eu0441u0442u0430u0432u043bu00a0u044eu0449u0438u0445.;4. a way to 2, in which the conversion from the time domain to the frequency (u0441u0442u0430u0434u0438u00a0 s2) u0432u044bu0447u0438u0441u043bu00a0u044eu0442 also u043eu043fu0440u0435u0434u0435u043bu00a0u0435u043cu044bu0439 sampling method of dft (c) and u043du0430u0445u043eu0434u00a0u0442 knowl u0447u0435u043du0438u00a0 his l different from u043du0443u043bu00a0 u0441u043eu0441u0442u0430u0432u043bu00a0u044eu0449u0438u0445.;5. method for p.1, in which case the u0434u0438u0441u043au0440u0435u0442u0438u0437u0438u0440u043eu0432u0430u043du043du044bu0439 signal x (tm) is presented in the form of pulses with u043du0435u0440u0435u0433u0443u043bu00a0u0440u043du044bu043c or u043du0435u043fu043eu0441u0442u043eu00a0u043du043du044bu043c period of their u043fu043eu0432u0442u043eu0440u0435u043du0438u00a0,between the end of u043eu0431u044au0435u0434u0438u043du0435u043du0438u00a0 impulses (u0441u0442u0430u0434u0438u00a0 S0) and phase u043fu0440u0435u043eu0431u0440u0430u0437u043eu0432u0430u043du0438u00a0 from time domain to frequency (u0441u0442u0430u0434u0438u00a0 s2) u043du0435u0440u0435u0433u0443u043bu00a0u0440u043du044bu0435 impulses - u043eu0442u0441u0447u0435u0442u044b x (tm) u0434u043eu043fu043eu043bu043du0438u0442u0435u043bu044cu043d on transforming the u0440u0435u0433u0443u043bu00a0u0440u043du044bu0435 impulses - u043eu0442u0441u0447u0435u0442u044b (r (iT) with the addition of missing values u043du0443u043bu00a0u043cu0438 (u0441u0442u0430u0434u0438u00a0 s1).;6. method for p.2, in which case the u0434u0438u0441u043au0440u0435u0442u0438u0437u0438u0440u043eu0432u0430u043du043du044bu0439 signal x (tm) is presented in the form of pulses with u043du0435u0440u0435u0433u0443u043bu00a0u0440u043du044bu043c or u043du0435u043fu043eu0441u0442u043eu00a0u043du043du044bu043c period of their u043fu043eu0432u0442u043eu0440u0435u043du0438u00a0,between the end of u043eu0431u044au0435u0434u0438u043du0435u043du0438u00a0 impulses (u0441u0442u0430u0434u0438u00a0 S0) and phase u043fu0440u0435u043eu0431u0440u0430u0437u043eu0432u0430u043du0438u00a0 from time domain to frequency (u0441u0442u0430u0434u0438u00a0 s2) u043du0435u0440u0435u0433u0443u043bu00a0u0440u043du044bu0435 impulses - u043eu0442u0441u0447u0435u0442u044b x (tm) u0434u043eu043fu043eu043bu043du0438u0442u0435u043bu044cu043d on transforming the u0440u0435u0433u0443u043bu00a0u0440u043du044bu0435 impulses - u043eu0442u0441u0447u0435u0442u044b (r (iT) with the addition of missing values u043du0443u043bu00a0u043cu0438 (u0441u0442u0430u0434u0438u00a0 s1).;7. method for p.3, in which case the u0434u0438u0441u043au0440u0435u0442u0438u0437u0438u0440u043eu0432u0430u043du043du044bu0439 signal x (tm) is presented in the form of pulses with u043du0435u0440u0435u0433u0443u043bu00a0u0440u043du044bu043c or u043du0435u043fu043eu0441u0442u043eu00a0u043du043du044bu043c period of their u043fu043eu0432u0442u043eu0440u0435u043du0438u00a0,between the end of u043eu0431u044au0435u0434u0438u043du0435u043du0438u00a0 impulses (u0441u0442u0430u0434u0438u00a0 S0) and phase u043fu0440u0435u043eu0431u0440u0430u0437u043eu0432u0430u043du0438u00a0 from time domain to frequency (u0441u0442u0430u0434u0438u00a0 s2) u043du0435u0440u0435u0433u0443u043bu00a0u0440u043du044bu0435 impulses - u043eu0442u0441u0447u0435u0442u044b x (tm) u0434u043eu043fu043eu043bu043du0438u0442u0435u043bu044cu043d on transforming the u0440u0435u0433u0443u043bu00a0u0440u043du044bu0435 impulses - u043eu0442u0441u0447u0435u0442u044b (r (iT) with the addition of missing values u043du0443u043bu00a0u043cu0438 (u0441u0442u0430u0434u0438u00a0 s1).;8. method for p.4, in which case the u0434u0438u0441u043au0440u0435u0442u0438u0437u0438u0440u043eu0432u0430u043du043du044bu0439 signal x (tm) is presented in the form of pulses with u043du0435u0440u0435u0433u0443u043bu00a0u0440u043du044bu043c or u043du0435u043fu043eu0441u0442u043eu00a0u043du043du044bu043c period of their u043fu043eu0432u0442u043eu0440u0435u043du0438u00a0,between the end of u043eu0431u044au0435u0434u0438u043du0435u043du0438u00a0 impulses (u0441u0442u0430u0434u0438u00a0 S0) and phase u043fu0440u0435u043eu0431u0440u0430u0437u043eu0432u0430u043du0438u00a0 from time domain to frequency (u0441u0442u0430u0434u0438u00a0 s2) u043du0435u0440u0435u0433u0443u043bu00a0u0440u043du044bu0435 impulses - u043eu0442u0441u0447u0435u0442u044b x (tm) additional but is in u0440u0435u0433u0443u043bu00a0u0440u043du044bu0435 impulses - u043eu0442u0441u0447u0435u0442u044b (r (iT) with the addition of missing values u043du0443u043bu00a0u043cu0438 (u0441u0442u0430u0434u0438u00a0 s1).;9. method for p.1, in which between the stage u043fu0440u0435u043eu0431u0440u0430u0437u043eu0432u0430u043du0438u00a0 from time domain to frequency (u0441u0442u0430u0434u0438u00a0 s2) and phase u0434u0435u043au043eu043du0432u043eu043bu044eu0446u0438u0438 (u0441u0442u0430u0434u0438u00a0 claims) further u0432u044bu0434u0435u043bu00a0u044eu0442 spectra to the otp u0430u0436u0435u043du0438u0439 under the assumption that these u043eu0442u0440u0430u0436u0435u043du0438u00a0 u0440u0430u0441u043fu0440u043eu0441u0442u0440u0430u043du00a0u044eu0442u0441u00a0 to more than a few calls impulses ranges (u0441u0442u0430u0434u0438u00a0 s3)the spectral line to the reflections on the basis of the average u0437u043du0430u0447u0435u043du0438u00a0 and width of their allocated spectrum (u0441u0442u0430u0434u0438u00a0 s4) and the measured spectra to the reflections u0432u044bu0447 u0438u0442u0430u044eu0442 of spectrum (u0441u0442u0430u0434u0438u00a0 s5).;10. the system u0434u043bu00a0 u0432u043eu0441u0441u0442u0430u043du043eu0432u043bu0435u043du0438u00a0 u0434u0438u0441u043au0440u0435u0442u0438u0437u0438u0440u043eu0432u0430u043du043du043eu0433u043e signal x (tm) in the form of periodic pulses that can be set u043fu043eu0432u0442u043eu0440u00a0u044eu0449u0438u0445u0441u00a0 with fast frequency u0438u043cu0435u044eu0449u0430u00a0 funds volume u0434u0438u043du0435u043du0438u00a0 between pulses with the same frequency as the load in the pack means u043fu0440u0435u043eu0431u0440u0430u0437u043eu0432u0430u043du0438u00a0 these impulses from time domain to frequency and means of u0434u0435u043au043eu043du0432 u043eu043bu044eu0446u0438u0438 obtained spectra.;11. the system p.10, u043au043eu0442u043eu0440u0430u00a0 also has means u043fu0440u0435u043eu0431u0440u0430u0437u043eu0432u0430u043du0438u00a0 u043du0435u0440u0435u0433u0443u043bu00a0u0440u043du044bu0445 impulses - u043eu0442u0441u0447u0435u0442u043eu0432 x (tm) in u0440u0435u0433u0443u043bu00a0u0440u043du044bu0435 impulses - u043eu0442u0441u0447u0435u0442u044b (r (iT) with the addition of missing values u043du0443u043bu00a0u043cu0438, p ri as means of u043fu0440u0435u043eu0431u0440u0430u0437u043eu0432u0430u043du0438u00a0 u043du0435u0440u0435u0433u0443u043bu00a0u0440u043du044bu0445 impulses - u043eu0442u0441u0447u0435u0442u043eu0432 in u0440u0435u0433u0443u043bu00a0u0440u043du044bu0435 receive u043du0435u0440u0435u0433u0443u043bu00a0u0440u043du044bu0435 impulses - u043eu0442u0441u0447u0435u0442u044b grouped into frequencyby means of u043eu0431u044au0435u0434u0438u043du0435u043du0438u00a0 pulses and transmit u0440u0435u0433u0443u043bu00a0u0440u043du044bu0435 impulses - u043eu0442u0441u0447u0435u0442u044b complementing the missing values in the transitional area from u043du0443u043bu00a0u043cu0438 u043fu0440u0435u043eu0431u0440u0430u0437u043eu0432u0430u043du0438u00a0 and in frequency.;12. the system p.10, u043au043eu0442u043eu0440u0430u00a0 is also located between the means of u043fu0440u0435u043eu0431u0440u0430u0437u043eu0432u0430u043du0438u00a0 from time domain to frequency u0434u0435u043au043eu043du0432u043eu043bu044eu0446u0438u0438 means and means u0432u044bu0434u0435u043bu0435u043du0438u00a0 spectra of mesh u0430u044eu0449u0438u0445 reflections in dft (r) under the assumption that these u043eu0442u0440u0430u0436u0435u043du0438u00a0 u0440u0430u0441u043fu0440u043eu0441u0442u0440u0430u043du00a0u044eu0442u0441u00a0 to more than a few calls pulses rangethe evaluation of spectral lines in the reflections on the basis of the average u0437u043du0430u0447u0435u043du0438u00a0 and width of their allocated funds from u0432u044bu0447u0438u0442u0430u043du0438u00a0 spectra and spectra of disturbing the total reflection of the total spectrum of the dft (r).;13. the system p.11, u043au043eu0442u043eu0440u0430u00a0 is also located between the means of u043fu0440u0435u043eu0431u0440u0430u0437u043eu0432u0430u043du0438u00a0 from time domain to frequency u0434u0435u043au043eu043du0432u043eu043bu044eu0446u0438u0438 means and means u0432u044bu0434u0435u043bu0435u043du0438u00a0 spectra of mesh u0430u044eu0449u0438u0445 reflections in dft (r) under the assumption that these u043eu0442u0440u0430u0436u0435u043du0438u00a0 u0440u0430u0441u043fu0440u043eu0441u0442u0440u0430u043du00a0u044eu0442u0441u00a0 to more than a few calls pulses rangethe evaluation of spectral lines in the reflections on the basis of the average u0437u043du0430u0447u0435u043du0438u00a0 and width of their allocated funds from u0432u044bu0447u0438u0442u0430u043du0438u00a0 spectra and spectra of disturbing the total reflection of the total spectrum of the dft (r).;14. u043fu0440u0438u0435u043cu043eu043fu0435u0440u0435u0434u0430u044eu0449u0430u00a0 system u0438u043cu0435u044eu0449u0430u00a0 antenna, a frequency generator, which is connected with the generator of a frequency synthesizer with frequency, connected to the er tim generator basic frequency synthesizer frequency u043fu043eu0432u0442u043eu0440u0435u043du0438u00a0 impulses, an analog-to-digital converter and a processor, which has the possibility of implementation u043bu0435u043du0438u00a0 method u0432u043eu0441u0441u0442u0430u043du043eu0432u043bu0435u043du0438u00a0 signal method u0434u0435u043au043eu043du0432u043eu043bu044eu0446u0438u0438 on 1.;15. u043fu0440u0438u0435u043cu043eu043fu0435u0440u0435u0434u0430u044eu0449u0430u00a0 system u0438u043cu0435u044eu0449u0430u00a0 antenna, a frequency generator, which is connected with the generator of a frequency synthesizer with frequency, connected to the er tim generator basic frequency synthesizer frequency u043fu043eu0432u0442u043eu0440u0435u043du0438u00a0 impulses, an analog-to-digital converter and a processor, which has the possibility of implementation u043bu0435u043du0438u00a0 method u0432u043eu0441u0441u0442u0430u043du043eu0432u043bu0435u043du0438u00a0 signal method u0434u0435u043au043eu043du0432u043eu043bu044eu0446u0438u0438 on p.2.;16. u043fu0440u0438u0435u043cu043eu043fu0435u0440u0435u0434u0430u044eu0449u0430u00a0 system u0438u043cu0435u044eu0449u0430u00a0 antenna, a frequency generator, which is connected with the generator of a frequency synthesizer with frequency, connected to the er tim generator basic frequency synthesizer frequency u043fu043eu0432u0442u043eu0440u0435u043du0438u00a0 impulses, an analog-to-digital converter and a processor, which has the possibility of implementation u043bu0435u043du0438u00a0 method u0432u043eu0441u0441u0442u0430u043du043eu0432u043bu0435u043du0438u00a0 signal method u0434u0435u043au043eu043du0432u043eu043bu044eu0446u0438u0438 on clause 5.;17. the application of the method u0432u043eu0441u0441u0442u0430u043du043eu0432u043bu0435u043du0438u00a0 signal method u0434u0435u043au043eu043du0432u043eu043bu044eu0446u0438u0438 on 1 in the radar system.;18. the application of the system u0434u043bu00a0 u0432u043eu0441u0441u0442u0430u043du043eu0432u043bu0435u043du0438u00a0 signal method u0434u0435u043au043eu043du0432u043eu043bu044eu0446u0438u0438 on p.10 in the radar system.;19. the application of u043fu0440u0438u0435u043cu043eu043fu0435u0440u0435u0434u0430u044eu0449u0435u0439 system on p.14 in the radar system.;20. the application of the method in paragraph 1 as a method of u043fu0440u043eu0442u0438u0432u043eu0434u0435u0439u0441u0442u0432u0438u00a0 active u0440u0430u0434u0438u043eu043fu043eu043cu0435u0445u0430u043c.
展开▼