jaxvacua.conifold.coniLCS_prepotential.F_coniLCS_exp_per#
- F_coniLCS_exp_per(self, X0, XConi, XPerBulk, conj=False, n=0)#
Computes the expansion of the prepotential \(F\) around the conifold point in terms of the periods.
Details
The prepotential \(F\) can be expanded around the conifold point as
\[F(X) = \sum_{n=0}^{\infty}\, \dfrac{1}{n!}\, \dfrac{\partial^n F}{\partial (X^{\mathrm{cf}})^n}\Bigg |_{X^{\mathrm{cf}}=0}\, (X^{\mathrm{cf}})^n\, .\]Here, \(X^{\mathrm{cf}}\) is the period associated to the conifold curve.
This function returns the coefficient of \((X^{\mathrm{cf}})^n\) in this expansion, i.e. it computes \(\tfrac{1}{n!}\,\partial^n_{\!X^{\mathrm{cf}}} F\big|_{X^{\mathrm{cf}}=0}\). The full coniLCS prepotential is reconstructed in
F_coniLCS_series_per()by summing these coefficients up to ordernmax.The individual contributions are:
- Polynomial part — obtained from
F_coniLCS_poly_split_per()and its derivatives
dF_coniLCS_poly_per(),ddF_coniLCS_poly_per(),dddF_coniLCS_poly_per()evaluated at \(X^{\mathrm{cf}}=0\).
- Polynomial part — obtained from
- Conifold part — the dilogarithm \(F_{\mathrm{coni}}\) contributes
Riemann zeta values at integer arguments: \(\zeta(3)\) at \(n=0\), \(\zeta(2)=\pi^2/6\) at \(n=1\), \(3/2\) at \(n=2\), and the Bernoulli numbers \(B_{n-2}\) for \(n \ge 3\).
- Worldsheet instantons — added via
F_inst_per_coni()when maximum_degree > 0.
- Worldsheet instantons — added via
- Parameters:
X0 (
complex) – Value of period \(X^0\).XConi (
complex) – Value of conifold period \(X^{\mathrm{cf}}\).XPerBulk (
Array) – Values of bulk periods \(X^i\).conj (
bool) – IfTrue, computes the complex conjugate. Defaults toFalse.n (
int) – Order of derivative. Defaults to0.
- Returns:
complex – Value of the \(n\)-th derivative of the prepotential \(F\) around the conifold point.
- Return type:
complex