From 652b32fdde9febd039fc0793eaf7b36aaab4bdbb Mon Sep 17 00:00:00 2001
From: guanjihuan <guanjihuan@163.com>
Date: Mon, 17 Mar 2025 16:23:18 +0800
Subject: [PATCH] Create eta_test_for_integral_of_DOS.py

---
 .../eta_test_for_integral_of_DOS.py           | 56 +++++++++++++++++++
 1 file changed, 56 insertions(+)
 create mode 100644 2025.03.17_eta_test_for_integral_of_DOS/eta_test_for_integral_of_DOS.py

diff --git a/2025.03.17_eta_test_for_integral_of_DOS/eta_test_for_integral_of_DOS.py b/2025.03.17_eta_test_for_integral_of_DOS/eta_test_for_integral_of_DOS.py
new file mode 100644
index 0000000..d1cde91
--- /dev/null
+++ b/2025.03.17_eta_test_for_integral_of_DOS/eta_test_for_integral_of_DOS.py
@@ -0,0 +1,56 @@
+"""
+This code is supported by the website: https://www.guanjihuan.com
+The newest version of this code is on the web page: https://www.guanjihuan.com/archives/45681
+"""
+
+import numpy as np
+
+def hamiltonian(width=2, length=2):   # 方格子哈密顿量
+    h = np.zeros((width*length, width*length))
+    # y方向的跃迁
+    for x in range(length):
+        for y in range(width-1):
+            h[x*width+y, x*width+y+1] = 1
+            h[x*width+y+1, x*width+y] = 1
+    # x方向的跃迁
+    for x in range(length-1):
+        for y in range(width):
+            h[x*width+y, (x+1)*width+y] = 1
+            h[(x+1)*width+y, x*width+y] = 1
+    return h
+
+# from numba import jit
+# @jit(nopython=True)
+def total_DOS_for_Fermi_energy_array(Fermi_energy_array, h, broadening):
+    dim_energy = Fermi_energy_array.shape[0]
+    dim = h.shape[0]
+    total_DOS_array = np.zeros((dim_energy))
+    i0 = 0
+    for Fermi_energy in Fermi_energy_array:
+        green = np.linalg.inv((Fermi_energy+broadening*1j)*np.eye(dim)-h)
+        total_DOS = -np.trace(np.imag(green))/np.pi # 通过格林函数求得总态密度
+        total_DOS_array[i0] = total_DOS
+        i0 += 1
+    return total_DOS_array
+
+def main():
+    plot_precision = 0.01 # 画图的精度/积分的精度
+    Fermi_energy_array = np.arange(-5, 5, plot_precision)
+    h = hamiltonian()
+    # import time
+    # begin_time = time.time()
+    for broadening in [0.5, 0.1, 0.01, 0.001, 0.0001]:
+        total_DOS_array = total_DOS_for_Fermi_energy_array(Fermi_energy_array, h, broadening)
+        sum_up = np.sum(total_DOS_array)*plot_precision
+        print(f'Broadening为{broadening}时的积分结果：{sum_up}')
+        # import matplotlib.pyplot as plt
+        # plt.plot(Fermi_energy_array, total_DOS_array/sum_up, '-o')
+        # plt.plot(Fermi_energy_array, total_DOS_array, '-o')  
+        # plt.xlabel('Fermi energy')
+        # plt.ylabel('Total DOS')
+        # plt.show()
+    # end_time = time.time()
+    # print(end_time-begin_time)
+
+if __name__ == '__main__':
+    main()
\ No newline at end of file