BRIEF DESCRIPTION OF THE DRAWINGS
The invention can be more fully understood by reading the subsequent detailed description and examples with references made to the accompanying drawings, wherein:
FIG. 1 shows a conventional modulation device;
FIG. 2 shows an embodiment of the invention;
FIG. 3 shows another embodiment of the invention; and
FIG. 4 illustrates the modulation calculation of the modulator of the invention.
DETAILED DESCRIPTION OF THE INVENTION
The following description is of the best-contemplated mode of carrying out the invention. This description is made for the purpose of illustrating the general principles of the invention and should not be taken in a limiting sense. The scope of the invention is best determined by reference to the appended claims.
FIG. 2 shows a harmonic-rejection modulation device 200 of the invention, which includes a frequency divider 204 having a frequency divider ratio, N, an initialization module 216, a phase splitter 218, a low pass filter 212, and a modulator 214. N is a positive real number. The frequency divider 204 converts signal 222 to a square wave 224 having duty cycle of 50%. The square wave 224 is the input signal of the phase splitter 218. The phase splitter 218 includes a first frequency divider 206, a second frequency divider 208, and a third frequency divider 210. The frequency divider ratio of the first frequency divider 206 is 3. The frequency divider ratios of the second and the third frequency dividers 208 and 210 are 2. In the harmonic-rejection modulation device 200, the frequency dividers 204, 206, 208 and 210 are implemented as D-flip-flops. The first frequency divider 206 generates four frequency-divided signals (conveyed by signal lines 226 and 228). The two frequency-divided signals in signal lines 226 have phase angles of 120° and 300°, respectively. The two frequency-divided signals in signal lines 228 have phase angles of 0° and 180°, respectively. Based on the frequency-divided signals (conveyed by signal lines 226) having phase angles of 120° and 300°, the second frequency divider 208 generates four unfiltered local oscillating signals (conveyed by signal lines 230) having phase angles of 30°, 120°, 210° and 300°, respectively. Based on the frequency-divided signals (conveyed by signal lines 228) having phase angles of 0° and 180°, the third frequency divider 210 generates four unfiltered local oscillating signals (conveyed by signal lines 232) having phase angle of 0°, 90°, 180° and 270°, respectively. The low pass filter 212 filters the high frequency components of the unfiltered local oscillating signals (having phase angles of 30°, 120°, 210°, 300°, 0°, 90°, 180°, and 270°, respectively) conveyed by signal lines 230 and 232 to generates eight local oscillating signals (conveyed by signal lines 234 and 236) for the modulator 214. The signal lines 234 convey the local oscillating signals having phase angles of 30°, 90°, 210°, and 270°, respectively. The signal lines 236 convey the local oscillating signals having phase angles of 0°, 120°, 180°, and 300°, respectively. Based on the local oscillating signals conveyed by the signal lines 234 and 236, the modulator 214 modulates the in-phase signal (I) and the quadrature phase (Q) of a baseband signal, wherein the third harmonics of the local oscillating signals (in signal lines 234 and 236) are eliminated in the modulation calculation of the modulator 214.
Before the modulation process of the harmonic-rejection modulation device 200, the initialization module 216 outputs a control signal 238 for the frequency divider 204 to hold the input signal 224 of the phase splitter 218, and then outputs an initialization signal 240 for the first, second, and third frequency dividers 206, 208 and 210 to configure the initial value thereof. If the first, second, and third frequency dividers 206, 208 and 210 are synchronized, the initialization module 216 outputs the control signal 238 again to trigger the frequency divider 204 to release the input signal 224 for the phase splitter 218.
The harmonic-rejection modulation device 200 improves modulation quality while precisely regulating amplitude of the square wave 224. The local oscillating signals conveyed by signal lines 234 and 236 have exact phase angle. The low pass filter 212 filters the high order harmonics of the unfiltered local oscillating signals (in 230 and 232) which are square waves. The third harmonics of the local oscillating signals (in 234 and 236) are eliminated in the modulation calculation of the modulator 214, such that no additional filter (as filter circuit 130) is required. Compared with the conventional modulation device 100, the harmonic-rejection modulation device 200 reduces production costs and power consumption while improving sideband suppression, carrier suppression, and undesired harmonic suppression.
FIG. 3 shows another embodiment of the invention, in which harmonic-rejection modulation device 300 includes a frequency divider 304 having a frequency divider ratio of N, an initialization module 316, a phase splitter 318, a low pass filter 312, and a modulator 314. The frequency divider 304 converts the signal 322 to a square wave 324 having a duty cycle of 50%. The square wave 324 is the input signal of the phase splitter 318. The difference between the harmonic-rejection modulation devices 200 and 300 is the architecture of the phase splitters 218 and 318. The phase splitter 318 includes a first frequency divider 306, a second frequency divider 308, and a third frequency divider 310. The frequency dividers 306, 308 and 310 are implemented as D-Flip-Flops. The frequency divided ratio of the first frequency divider 306 is 2. The frequency divider ratios of the second and the third frequency dividers 308 and 310 are 3. Based on the square wave 324, the first frequency divider 306 generates four frequency-divided signals having phase angles of 0°, 90°, 180°, and 270°, respectively. Signal lines 326 convey the frequency-divided signals having phase angles of 90° and 270°. Signal lines 328 convey the frequency-divided signals having phase angles of 0° and 180°. Based on the frequency-divided signals (in the signal lines 326) having phase angles of 90° and 270°, the second frequency divider 308 generates four unfiltered local oscillating signals (conveyed by signal lines 330) having phase angles of 30°, 90°, 210°, and 270°, respectively. Based on the frequency-divided signals (in the signal lines 328) having phase angles of 0° and 180°, the third frequency divider 310 generates four unfiltered local oscillating signals (conveyed by signal lines 332) having phase angles of 0°, 120°, 180°, and 300°, respectively. The low pass filter 312 filters the high frequency components of the unfiltered local oscillating signals (in the signal lines 330 and 332) having phase angles of 30°, 90°, 210°, 270°, 0°, 120°, 180°, and 300° to generate local oscillating signals (conveyed by signal lines 334 and 336). The signal lines 334 convey the local oscillating signals having phase angles of 30°, 90°, 210°, and 270°. The signal lines 336 convey the local oscillating signals having phase angles of 0°, 120°, 180°, and 300°. Based on the local oscillating signals conveyed by the signal lines 334 and 336, the modulator 314 modulates the in-phase signal (I) and the quadrature phase (Q) of a baseband signal, wherein the third harmonics of the local oscillating signals (conveyed by the signal lines 334 and 336) are eliminated in the modulation calculation of the modulator 314. The modulator 314 is similar to the modulator 214 shown in FIG. 2.
Before the modulation process of the harmonic-rejection modulation device 300, the initialization module 316 outputs a control signal 338 for the frequency divider 304 to hold the input signal 324 of the phase splitter 318, and then outputs an initialization signal 340 to configure the initial value of the first, second, and third frequency dividers 306, 308 and 310. If the first, second, and third frequency dividers 306, 308, and 310 are synchronized, the initialization module 316 outputs the control signal 338 to again trigger the frequency divider 304 to release the input signal 324 for the phase splitter 318.
FIG. 4 illustrates modulation calculation of the modulator 214. Based on the local oscillating signals conveyed by signal lines 234 and 236, the modulator modulates the in-phase signal (I) and the quadrature phase (Q) of a baseband signal, wherein the third harmonics of the local oscillating signals (in signal lines 234 and 236) are eliminated by modulation calculation of the modulator 214. As shown in FIG. 4, the signals 402, 404, 410 and 412 are the local oscillating signals (in the signal lines 234) having phase angles of 210°, 270°, 30°, and 90°, respectively. The signals 406, 408, 414 and 416 are the local oscillating signals (in the signal lines 236) having phase angles of 300°, 0°, 120°, and 180°, respectively. As an example, the in-phase signal (I) of a baseband signal is cos(wbbt), and the quadrature phase signal (Q) of the baseband signal is sin(wbbt). Because the high-order harmonics are reduced by the low pass filter 212, the local oscillating signals 402, 404, 406, 408, 410, 412, 414 and 416 can be simplified as cos(wlot−150)+cos(3wlot−450)/3, cos(wlot−90)+cos(3wlot−270)/3, cos(wlot−60)+cos(3wlot−180)/3, cos(wlot)+cos(3wlot)/3, cos(wlot+30)+cos(3wlot+90)/3, cos(wlot+90)+cos(3wlot+270)/3, cos(wlot+120)+cos(3wlot+360)/3 and cos(wlot−180)+cos(3wlot−540)/3, respectively, which can be further simplified as sin(wlot−60)+cos(3wlot)/3, sin(wlot)−sin(3wlot)/3, cos(wlot−60)−cos(3wlot)/3, cos(wlot)+cos(3wlot)/3, cos(wlot+30)−sin(3wlot)/3, sin(wlot)+sin(3wlot)/3, −sin(wlot+30)+cos(3wlot)/3 and −cos(wlot)−cos(3wlot)/3, respectively. Only the first and the third order harmonics of the local oscillating signals need be considered. As shown in the upper part of FIG. 4, the in-phase signal (I) and the quadrature phase signal (Q) of the baseband signal are modulated by the local oscillating signals 402, 404, 406 and 408 to generate a first modulation signal 422, cos(wbbt)[sin(wlot−60)+sin(wlot)]+sin(wbbt)[cos(wlot)+cos(wlot−60)]. As shown in the lower part of FIG. 4, the in-phase signal (I) and the quadrature phase signal (Q) of the baseband signal are modulated by the local oscillating signals 410, 412, 414 and 416 to generate a second modulation signal 424, cos(wbbt)[cos(wlot+30)−sin(wlot)]+sin(wbbt)[−sin(wlot+30)−cos(wlot)]. The third harmonics of the local oscillating signals 402 to 416 are thus eliminated from the modulation calculation of the modulator 214.
The phase splitter 218 or 318 is utilized to generate local oscillating signals having phase angles of 0°, 30°, 90°, 120°, 180°, 210°, 270° and 300°. Any device capable of generating local oscillating signals having the same phase angles may replace the phase splitter of the harmonic-rejection modulation device of the invention. The third harmonics of these specific local oscillating signals can be successfully eliminated by the modulation calculation of the modulator disclosed.
While the invention has been described by way of example and in terms of preferred embodiment, it is to be understood that the invention is not limited thereto. To the contrary, it is intended to cover various modifications and similar arrangements (as would be apparent to those skilled in the art). Therefore, the scope of the appended claims should be accorded to the broadest interpretation so as to encompass all such modifications and similar arrangements.
Patent Application
20070242775
