Skip to content

Commit 5b5dccd

Browse files
authored
Update index.md
1 parent f90b8a8 commit 5b5dccd

File tree

1 file changed

+2
-0
lines changed

1 file changed

+2
-0
lines changed

docs/index.md

+2
Original file line numberDiff line numberDiff line change
@@ -226,6 +226,7 @@ from math import pi, sin, cos, sqrt
226226
**1.1 Write a Haldane model Hamiltonian on a hexagonal lattice, given the following parameters: wavevector components $k_x$ and $k_y$ (momentum) in the x and y directions, lattice spacing $a$, nearest-neighbor coupling constant $t_1$, next-nearest-neighbor coupling constant $t_2$, phase $\phi$ for the next-nearest-neighbor hopping, and the on-site energy $m$.**
227227

228228
**_Scientists Annotated Background:_**
229+
229230
Source: Haldane, F. D. M. (1988). Model for a quantum Hall effect without Landau levels: Condensed-matter realization of the" parity anomaly". Physical review letters, 61(18).
230231

231232
We denote $\{\mathbf{a}_i\}$ are the vectors from a B site to its three nearest-neighbor A sites, and $\{\mathbf{b}_i\}$ are next-nearest-neighbor distance vectors, then we have
@@ -338,6 +339,7 @@ assert np.allclose(calc_hamiltonian(kx, ky, a, t1, t2, phi, m), target)
338339
**1.2 Calculate the Chern number using the Haldane Hamiltonian, given the grid size $\delta$ for discretizing the Brillouin zone in the $k_x$ and $k_y$ directions (assuming the grid sizes are the same in both directions), the lattice spacing $a$, the nearest-neighbor coupling constant $t_1$, the next-nearest-neighbor coupling constant $t_2$, the phase $\phi$ for the next-nearest-neighbor hopping, and the on-site energy $m$.**
339340

340341
**_Scientists Annotated Background:_**
342+
341343
Source: Fukui, Takahiro, Yasuhiro Hatsugai, and Hiroshi Suzuki. "Chern numbers in discretized Brillouin zone: efficient method of computing (spin) Hall conductances." Journal of the Physical Society of Japan 74.6 (2005): 1674-1677.
342344

343345

0 commit comments

Comments
 (0)