From dffafbb61ee7424991ab7480842c4ebfa7b790da Mon Sep 17 00:00:00 2001
From: guanjihuan <guanjihuan@163.com>
Date: Sun, 9 Oct 2022 02:51:02 +0800
Subject: [PATCH] update

---
 .../Wilson_loop_in_SSH_model.py                                 | 2 +-
 .../Wilson_loop_in_SSH_model_with_better_code.py                | 2 +-
 ...graphene_under_broken_inversion_symmery_with_Kubo_formula.py | 2 +-
 ..._graphene_under_broken_inversion_symmery_with_Wilson_loop.py | 2 +-
 ..._under_broken_inversion_symmery_with_the_efficient_method.py | 2 +-
 ...y_curvature_distribution_with_Wilson_loop_(function_form).py | 2 +-
 ...tion_with_Wilson_loop_for_degenerate_case_(function_form).py | 2 +-
 ...re_distribution_with_the_efficient_method_(function_form).py | 2 +-
 ..._the_efficient_method_for_degenerate_case_(function_form).py | 2 +-
 9 files changed, 9 insertions(+), 9 deletions(-)

diff --git a/academic_codes/2021.03.01_Wilson_loop_in_SSH_model/Wilson_loop_in_SSH_model.py b/academic_codes/2021.03.01_Wilson_loop_in_SSH_model/Wilson_loop_in_SSH_model.py
index 5681eb9..0177fbc 100755
--- a/academic_codes/2021.03.01_Wilson_loop_in_SSH_model/Wilson_loop_in_SSH_model.py
+++ b/academic_codes/2021.03.01_Wilson_loop_in_SSH_model/Wilson_loop_in_SSH_model.py
@@ -11,7 +11,7 @@ from math import *
 def hamiltonian(k):  # SSH模型哈密顿量
     gamma = 0.5
     lambda0 = 1
-    h = np.zeros((2, 2))*(1+0j)
+    h = np.zeros((2, 2), dtype=complex)
     h[0,0] = 0
     h[1,1] = 0
     h[0,1] = gamma+lambda0*cmath.exp(-1j*k)
diff --git a/academic_codes/2021.03.01_Wilson_loop_in_SSH_model/Wilson_loop_in_SSH_model_with_better_code.py b/academic_codes/2021.03.01_Wilson_loop_in_SSH_model/Wilson_loop_in_SSH_model_with_better_code.py
index 96f9931..adfc149 100755
--- a/academic_codes/2021.03.01_Wilson_loop_in_SSH_model/Wilson_loop_in_SSH_model_with_better_code.py
+++ b/academic_codes/2021.03.01_Wilson_loop_in_SSH_model/Wilson_loop_in_SSH_model_with_better_code.py
@@ -12,7 +12,7 @@ def hamiltonian(k):
     gamma = 0.5
     lambda0 = 1
     delta = 0
-    h = np.zeros((2, 2))*(1+0j)
+    h = np.zeros((2, 2), dtype=complex)
     h[0,0] = delta
     h[1,1] = -delta
     h[0,1] = gamma+lambda0*cmath.exp(-1j*k)
diff --git a/academic_codes/2022.04.21_Berry_curvature/Berry_curvature_distribution_of_graphene_under_broken_inversion_symmery_with_Kubo_formula.py b/academic_codes/2022.04.21_Berry_curvature/Berry_curvature_distribution_of_graphene_under_broken_inversion_symmery_with_Kubo_formula.py
index 2ea3bbb..1cd68e8 100644
--- a/academic_codes/2022.04.21_Berry_curvature/Berry_curvature_distribution_of_graphene_under_broken_inversion_symmery_with_Kubo_formula.py
+++ b/academic_codes/2022.04.21_Berry_curvature/Berry_curvature_distribution_of_graphene_under_broken_inversion_symmery_with_Kubo_formula.py
@@ -10,7 +10,7 @@ import cmath
 
 
 def hamiltonian(k1, k2, t1=2.82, a=1/sqrt(3)):  # 石墨烯哈密顿量（a为原子间距，不赋值的话默认为1/sqrt(3)）
-    h = np.zeros((2, 2))*(1+0j)
+    h = np.zeros((2, 2), dtype=complex)
     h[0, 0] = 0.28/2
     h[1, 1] = -0.28/2
     h[1, 0] = t1*(cmath.exp(1j*k2*a)+cmath.exp(1j*sqrt(3)/2*k1*a-1j/2*k2*a)+cmath.exp(-1j*sqrt(3)/2*k1*a-1j/2*k2*a))
diff --git a/academic_codes/2022.04.21_Berry_curvature/Berry_curvature_distribution_of_graphene_under_broken_inversion_symmery_with_Wilson_loop.py b/academic_codes/2022.04.21_Berry_curvature/Berry_curvature_distribution_of_graphene_under_broken_inversion_symmery_with_Wilson_loop.py
index d9093fd..9b6699b 100644
--- a/academic_codes/2022.04.21_Berry_curvature/Berry_curvature_distribution_of_graphene_under_broken_inversion_symmery_with_Wilson_loop.py
+++ b/academic_codes/2022.04.21_Berry_curvature/Berry_curvature_distribution_of_graphene_under_broken_inversion_symmery_with_Wilson_loop.py
@@ -10,7 +10,7 @@ import cmath
 
 
 def hamiltonian(k1, k2, t1=2.82, a=1/sqrt(3)):  # 石墨烯哈密顿量（a为原子间距，不赋值的话默认为1/sqrt(3)）
-    h = np.zeros((2, 2))*(1+0j)
+    h = np.zeros((2, 2), dtype=complex)
     h[0, 0] = 0.28/2
     h[1, 1] = -0.28/2
     h[1, 0] = t1*(cmath.exp(1j*k2*a)+cmath.exp(1j*sqrt(3)/2*k1*a-1j/2*k2*a)+cmath.exp(-1j*sqrt(3)/2*k1*a-1j/2*k2*a))
diff --git a/academic_codes/2022.04.21_Berry_curvature/Berry_curvature_distribution_of_graphene_under_broken_inversion_symmery_with_the_efficient_method.py b/academic_codes/2022.04.21_Berry_curvature/Berry_curvature_distribution_of_graphene_under_broken_inversion_symmery_with_the_efficient_method.py
index 340d523..f120582 100644
--- a/academic_codes/2022.04.21_Berry_curvature/Berry_curvature_distribution_of_graphene_under_broken_inversion_symmery_with_the_efficient_method.py
+++ b/academic_codes/2022.04.21_Berry_curvature/Berry_curvature_distribution_of_graphene_under_broken_inversion_symmery_with_the_efficient_method.py
@@ -10,7 +10,7 @@ import cmath
 
 
 def hamiltonian(k1, k2, t1=2.82, a=1/sqrt(3)):  # 石墨烯哈密顿量（a为原子间距，不赋值的话默认为1/sqrt(3)）
-    h = np.zeros((2, 2))*(1+0j)
+    h = np.zeros((2, 2), dtype=complex)
     h[0, 0] = 0.28/2
     h[1, 1] = -0.28/2
     h[1, 0] = t1*(cmath.exp(1j*k2*a)+cmath.exp(1j*sqrt(3)/2*k1*a-1j/2*k2*a)+cmath.exp(-1j*sqrt(3)/2*k1*a-1j/2*k2*a))
diff --git a/academic_codes/2022.08.13_Berry_curvature_distribution_in_function_form/Berry_curvature_distribution_with_Wilson_loop_(function_form).py b/academic_codes/2022.08.13_Berry_curvature_distribution_in_function_form/Berry_curvature_distribution_with_Wilson_loop_(function_form).py
index b882254..a62c656 100644
--- a/academic_codes/2022.08.13_Berry_curvature_distribution_in_function_form/Berry_curvature_distribution_with_Wilson_loop_(function_form).py
+++ b/academic_codes/2022.08.13_Berry_curvature_distribution_in_function_form/Berry_curvature_distribution_with_Wilson_loop_(function_form).py
@@ -10,7 +10,7 @@ import math
 
 
 def hamiltonian(k1, k2, t1=2.82, a=1/sqrt(3)):  # 石墨烯哈密顿量（a为原子间距，不赋值的话默认为1/sqrt(3)）
-    h = np.zeros((2, 2))*(1+0j)
+    h = np.zeros((2, 2), dtype=complex)
     h[0, 0] = 0.28/2
     h[1, 1] = -0.28/2
     h[1, 0] = t1*(cmath.exp(1j*k2*a)+cmath.exp(1j*sqrt(3)/2*k1*a-1j/2*k2*a)+cmath.exp(-1j*sqrt(3)/2*k1*a-1j/2*k2*a))
diff --git a/academic_codes/2022.08.13_Berry_curvature_distribution_in_function_form/Berry_curvature_distribution_with_Wilson_loop_for_degenerate_case_(function_form).py b/academic_codes/2022.08.13_Berry_curvature_distribution_in_function_form/Berry_curvature_distribution_with_Wilson_loop_for_degenerate_case_(function_form).py
index 34e2d44..fb59291 100644
--- a/academic_codes/2022.08.13_Berry_curvature_distribution_in_function_form/Berry_curvature_distribution_with_Wilson_loop_for_degenerate_case_(function_form).py
+++ b/academic_codes/2022.08.13_Berry_curvature_distribution_in_function_form/Berry_curvature_distribution_with_Wilson_loop_for_degenerate_case_(function_form).py
@@ -10,7 +10,7 @@ import math
 
 
 def hamiltonian(k1, k2, t1=2.82, a=1/sqrt(3)):  # 石墨烯哈密顿量（a为原子间距，不赋值的话默认为1/sqrt(3)）
-    h = np.zeros((2, 2))*(1+0j)
+    h = np.zeros((2, 2), dtype=complex)
     h[0, 0] = 0.28/2
     h[1, 1] = -0.28/2
     h[1, 0] = t1*(cmath.exp(1j*k2*a)+cmath.exp(1j*sqrt(3)/2*k1*a-1j/2*k2*a)+cmath.exp(-1j*sqrt(3)/2*k1*a-1j/2*k2*a))
diff --git a/academic_codes/2022.08.13_Berry_curvature_distribution_in_function_form/Berry_curvature_distribution_with_the_efficient_method_(function_form).py b/academic_codes/2022.08.13_Berry_curvature_distribution_in_function_form/Berry_curvature_distribution_with_the_efficient_method_(function_form).py
index 9002431..2cc5c18 100644
--- a/academic_codes/2022.08.13_Berry_curvature_distribution_in_function_form/Berry_curvature_distribution_with_the_efficient_method_(function_form).py
+++ b/academic_codes/2022.08.13_Berry_curvature_distribution_in_function_form/Berry_curvature_distribution_with_the_efficient_method_(function_form).py
@@ -9,7 +9,7 @@ import cmath
 import math
 
 def hamiltonian(k1, k2, t1=2.82, a=1/sqrt(3)):  # 石墨烯哈密顿量（a为原子间距，不赋值的话默认为1/sqrt(3)）
-    h = np.zeros((2, 2))*(1+0j)
+    h = np.zeros((2, 2), dtype=complex)
     h[0, 0] = 0.28/2
     h[1, 1] = -0.28/2
     h[1, 0] = t1*(cmath.exp(1j*k2*a)+cmath.exp(1j*sqrt(3)/2*k1*a-1j/2*k2*a)+cmath.exp(-1j*sqrt(3)/2*k1*a-1j/2*k2*a))
diff --git a/academic_codes/2022.08.13_Berry_curvature_distribution_in_function_form/Berry_curvature_distribution_with_the_efficient_method_for_degenerate_case_(function_form).py b/academic_codes/2022.08.13_Berry_curvature_distribution_in_function_form/Berry_curvature_distribution_with_the_efficient_method_for_degenerate_case_(function_form).py
index f92097b..b17350c 100644
--- a/academic_codes/2022.08.13_Berry_curvature_distribution_in_function_form/Berry_curvature_distribution_with_the_efficient_method_for_degenerate_case_(function_form).py
+++ b/academic_codes/2022.08.13_Berry_curvature_distribution_in_function_form/Berry_curvature_distribution_with_the_efficient_method_for_degenerate_case_(function_form).py
@@ -10,7 +10,7 @@ import math
 
 
 def hamiltonian(k1, k2, t1=2.82, a=1/sqrt(3)):  # 石墨烯哈密顿量（a为原子间距，不赋值的话默认为1/sqrt(3)）
-    h = np.zeros((2, 2))*(1+0j)
+    h = np.zeros((2, 2), dtype=complex)
     h[0, 0] = 0.28/2
     h[1, 1] = -0.28/2
     h[1, 0] = t1*(cmath.exp(1j*k2*a)+cmath.exp(1j*sqrt(3)/2*k1*a-1j/2*k2*a)+cmath.exp(-1j*sqrt(3)/2*k1*a-1j/2*k2*a))