Spin-quadrupole coefficients

Phase term Exact expression inside 3/(128 eta v^5) Evidence
Q4 \(- 50 \cdot \chi_{1}^{2} \cdot \left(C_{Q1} - 1\right) \cdot \left(\frac{\delta}{2} + \frac{1}{2}\right)^{2} - 50 \cdot \chi_{2}^{2} \cdot \left(\frac{1}{2} - \frac{\delta}{2}\right)^{2} \cdot \left(C_{Q2} - 1\right)\) nagar2018, Eq. 2, 38, 44, 50
Q6 \(\frac{2215 \cdot \delta \cdot \left(\chi_{1}^{2} \cdot \left(C_{Q1} - 1\right) \cdot \left(\frac{\delta}{2} + \frac{1}{2}\right)^{2} - \chi_{2}^{2} \cdot \left(\frac{1}{2} - \frac{\delta}{2}\right)^{2} \cdot \left(C_{Q2} - 1\right)\right)}{12} + \left(\frac{16265}{21} - 30 \cdot \delta^{2}\right) \cdot \left(\chi_{1}^{2} \cdot \left(C_{Q1} - 1\right) \cdot \left(\frac{\delta}{2} + \frac{1}{2}\right)^{2} + \chi_{2}^{2} \cdot \left(\frac{1}{2} - \frac{\delta}{2}\right)^{2} \cdot \left(C_{Q2} - 1\right)\right)\) nagar2018, Eq. 2, 38, 46, 51
Q7_tail \(- 400 \cdot \pi \cdot \left(\chi_{1}^{2} \cdot \left(C_{Q1} - 1\right) \cdot \left(\frac{\delta}{2} + \frac{1}{2}\right)^{2} + \chi_{2}^{2} \cdot \left(\frac{1}{2} - \frac{\delta}{2}\right)^{2} \cdot \left(C_{Q2} - 1\right)\right)\) nagar2018, Eq. 2, 38, 47, 52
Q7_cubic \(10 \cdot \chi_{1}^{2} \cdot \left(C_{Q1} - 1\right) \cdot \left(\frac{\delta}{2} + \frac{1}{2}\right)^{2} \cdot \left(\chi_{1} \cdot \left(\frac{154 \cdot \delta}{3} + \left(\frac{\delta}{2} + \frac{1}{2}\right)^{2} + \frac{154}{3}\right) + \chi_{2} \cdot \left(\frac{89 \cdot \delta}{6} + \left(\frac{1}{2} - \frac{\delta}{2}\right)^{2} - \frac{89}{6}\right)\right) + 10 \cdot \chi_{2}^{2} \cdot \left(\frac{1}{2} - \frac{\delta}{2}\right)^{2} \cdot \left(C_{Q2} - 1\right) \cdot \left(\chi_{1} \cdot \left(- \frac{89 \cdot \delta}{6} + \left(\frac{\delta}{2} + \frac{1}{2}\right)^{2} - \frac{89}{6}\right) + \chi_{2} \cdot \left(- \frac{154 \cdot \delta}{3} + \left(\frac{1}{2} - \frac{\delta}{2}\right)^{2} + \frac{154}{3}\right)\right)\) dietrich2019, Eq. 26, 27