Table 3 GLPSM coding coefficients for NT = 8
From: Multiple transmit antennas for low PAPR spatial modulation in SC-FDMA: single vs. multiple streams
t = 1 | t = 2 | t = 3 | t = 4 | t = 5 | t = 6 | t = 7 | t = 8 | |
|---|---|---|---|---|---|---|---|---|
p = 0 | \( \sqrt{\frac{1}{8}} \) | \( \sqrt{\frac{1}{8}} \) | \( \sqrt{\frac{1}{8}} \) | \( \sqrt{\frac{1}{8}} \) | \( \sqrt{\frac{1}{8}} \) | \( \sqrt{\frac{1}{8}} \) | \( \sqrt{\frac{1}{8}} \) | \( \sqrt{\frac{1}{8}} \) |
p = 1 | \( \sqrt{\frac{1}{8}} \) | \( \sqrt{\frac{1}{8}}{e}^{j\frac{\uppi}{4}} \) | \( \sqrt{\frac{1}{8}}{e}^{j\frac{\uppi}{2}} \) | \( \sqrt{\frac{1}{8}}{e}^{j\frac{3\uppi}{4}} \) | \( -\sqrt{\frac{1}{8}} \) | \( \sqrt{\frac{1}{8}}{e}^{j\frac{5\uppi}{4}} \) | \( \sqrt{\frac{1}{8}}{e}^{j\frac{3\uppi}{2}} \) | \( \sqrt{\frac{1}{8}}{e}^{j\frac{7\uppi}{4}} \) |
p = 2 | \( \sqrt{\frac{1}{8}} \) | \( \sqrt{\frac{1}{8}}{e}^{j\frac{\uppi}{2}} \) | \( -\sqrt{\frac{1}{8}} \) | \( \sqrt{\frac{1}{8}}{e}^{j\frac{3\uppi}{2}} \) | \( \sqrt{\frac{1}{8}} \) | \( \sqrt{\frac{1}{8}}{e}^{j\frac{\uppi}{2}} \) | \( -\sqrt{\frac{1}{8}} \) | \( \sqrt{\frac{1}{8}}{e}^{j\frac{3\uppi}{2}} \) |
p = 3 | \( \sqrt{\frac{1}{8}} \) | \( \sqrt{\frac{1}{8}}{e}^{j\frac{3\uppi}{4}} \) | \( \sqrt{\frac{1}{8}}{e}^{j\frac{3\uppi}{2}} \) | \( \sqrt{\frac{1}{8}}{e}^{j\frac{\uppi}{4}} \) | \( -\sqrt{\frac{1}{8}} \) | \( \sqrt{\frac{1}{8}}{e}^{j\frac{7\uppi}{4}} \) | \( \sqrt{\frac{1}{8}}{e}^{j\frac{\uppi}{2}} \) | \( \sqrt{\frac{1}{8}}{e}^{j\frac{5\uppi}{4}} \) |
p = 4 | \( \sqrt{\frac{1}{8}} \) | \( -\sqrt{\frac{1}{8}} \) | \( \sqrt{\frac{1}{8}} \) | \( -\sqrt{\frac{1}{8}} \) | \( \sqrt{\frac{1}{8}} \) | \( -\sqrt{\frac{1}{8}} \) | \( \sqrt{\frac{1}{8}} \) | \( -\sqrt{\frac{1}{8}} \) |
p = 5 | \( \sqrt{\frac{1}{8}} \) | \( \sqrt{\frac{1}{8}}{e}^{j\frac{5\uppi}{4}} \) | \( \sqrt{\frac{1}{8}}{e}^{j\frac{\uppi}{2}} \) | \( \sqrt{\frac{1}{8}}{e}^{j\frac{7\uppi}{4}} \) | \( -\sqrt{\frac{1}{8}} \) | \( \sqrt{\frac{1}{8}}{e}^{j\frac{\uppi}{4}} \) | \( \sqrt{\frac{1}{8}}{e}^{j\frac{3\uppi}{2}} \) | \( \sqrt{\frac{1}{8}}{e}^{j\frac{3\uppi}{4}} \) |
p = 6 | \( \sqrt{\frac{1}{8}} \) | \( \sqrt{\frac{1}{8}}{e}^{j\frac{3\uppi}{2}} \) | \( -\sqrt{\frac{1}{8}} \) | \( \sqrt{\frac{1}{8}}{e}^{j\frac{\uppi}{2}} \) | \( \sqrt{\frac{1}{8}} \) | \( \sqrt{\frac{1}{8}}{e}^{j\frac{3\uppi}{2}} \) | \( -\sqrt{\frac{1}{8}} \) | \( \sqrt{\frac{1}{8}}{e}^{j\frac{\uppi}{2}} \) |
p = 7 | \( \sqrt{\frac{1}{8}} \) | \( \sqrt{\frac{1}{8}}{e}^{j\frac{7\uppi}{4}} \) | \( \sqrt{\frac{1}{8}}{e}^{j\frac{3\uppi}{2}} \) | \( \sqrt{\frac{1}{8}}{e}^{j\frac{5\uppi}{4}} \) | \( -\sqrt{\frac{1}{8}} \) | \( \sqrt{\frac{1}{8}}{e}^{j\frac{3\uppi}{4}} \) | \( \sqrt{\frac{1}{8}}{e}^{j\frac{\uppi}{2}} \) | \( \sqrt{\frac{1}{8}}{e}^{j\frac{\uppi}{4}} \) |