From a5839806eb368ea4d2fe41e974799abaf20788b8 Mon Sep 17 00:00:00 2001
From: Johanna <johanna@zijderveld.de>
Date: Tue, 7 May 2024 15:50:37 +0200
Subject: [PATCH] fix renames of functions
---
docs/source/graphene_example.md | 2 +-
docs/source/hubbard_1d.md | 2 +-
2 files changed, 2 insertions(+), 2 deletions(-)
diff --git a/docs/source/graphene_example.md b/docs/source/graphene_example.md
index 1931a9a..cd3a265 100644
--- a/docs/source/graphene_example.md
+++ b/docs/source/graphene_example.md
@@ -70,7 +70,7 @@ We can now create a phase diagram of the gap of the interacting solution. In ord
```{code-cell} ipython3
def compute_gap(h, fermi_energy=0, nk=100):
- kham = pymf.tb_to_khamvector(h, nk, ks=None)
+ kham = pymf.tb_to_kgrid(h, nk)
vals = np.linalg.eigvalsh(kham)
emax = np.max(vals[vals <= fermi_energy])
diff --git a/docs/source/hubbard_1d.md b/docs/source/hubbard_1d.md
index 8f1a7ea..9c5b75e 100644
--- a/docs/source/hubbard_1d.md
+++ b/docs/source/hubbard_1d.md
@@ -42,7 +42,7 @@ We verify this tight-binding model by plotting the band structure and observing
# Set number of k-points
nk = 100
ks = np.linspace(0, 2*np.pi, nk, endpoint=False)
-hamiltonians_0 = pymf.tb_to_khamvector(h_0, nk, ks=ks)
+hamiltonians_0 = pymf.tb_to_kgrid(h_0, nk)
vals, vecs = np.linalg.eigh(hamiltonians_0)
plt.plot(ks, vals, c="k")
--
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