diff --git a/examples/linac_segment/README.rst b/examples/linac_segment/README.rst
index 58e0d4ea4..d44e48aa5 100644
--- a/examples/linac_segment/README.rst
+++ b/examples/linac_segment/README.rst
@@ -1,7 +1,7 @@
 .. _examples-linac-segment:
 
 PIP-II Linac Segment
-=======================
+====================
 
 This example illustrates a small segment of the PIP-II linac, which includes the last RF cavity in the MEBT section (a quarter-wave resonator cavity for longitudinal bunching) and the first
 RF cavity in the succeeding cryomodule (a superconducting half-wave resonator for acceleration).
diff --git a/examples/linac_segment/analysis_linac_segment.py b/examples/linac_segment/analysis_linac_segment.py
index 8905584df..1f483786b 100755
--- a/examples/linac_segment/analysis_linac_segment.py
+++ b/examples/linac_segment/analysis_linac_segment.py
@@ -1,6 +1,6 @@
 #!/usr/bin/env python3
 #
-# Copyright 2022-2023 ImpactX contributors
+# Copyright 2022-2025 ImpactX contributors
 # Authors: Axel Huebl, Chad Mitchell
 # License: BSD-3-Clause-LBNL
 #
diff --git a/examples/linac_segment/input_linac_segment.in b/examples/linac_segment/input_linac_segment.in
index 4d75e353d..920262c55 100644
--- a/examples/linac_segment/input_linac_segment.in
+++ b/examples/linac_segment/input_linac_segment.in
@@ -2,7 +2,7 @@
 ###############################################################################
 # Particle Beam(s)
 ###############################################################################
-#beam.npart = 10000000  #use this value for high-resolution runs
+#beam.npart = 10000000  # use this value for high-resolution runs
 beam.npart = 10000
 beam.units = static
 beam.kin_energy = 2.1226695
@@ -262,7 +262,7 @@ SOL2b.sin_coefficients = \
           -1.3824319466948509E-009 \
           -2.3654450397774321E-008 \
           -2.3981556296348572E-008 \
-           -4.3793988876300594E-008 \
+          -4.3793988876300594E-008 \
            5.3089692633387364E-009 \
            6.5186324602062307E-009 \
            3.9130100049078465E-008 \
@@ -363,7 +363,7 @@ algo.space_charge = true
 
 # Space charge using IGF solver
 algo.poisson_solver = "fft"
-#amr.n_cell = 64 64 64  #use this value for high resolution runs
+#amr.n_cell = 64 64 64  # use this value for high resolution runs
 amr.n_cell = 32 32 32
 geometry.prob_relative = 1.1 1.1
 
diff --git a/examples/linac_segment/run_linac_segment.py b/examples/linac_segment/run_linac_segment.py
index ef3776100..392280056 100644
--- a/examples/linac_segment/run_linac_segment.py
+++ b/examples/linac_segment/run_linac_segment.py
@@ -1,7 +1,7 @@
 #!/usr/bin/env python3
 #
-# Copyright 2022-2024 ImpactX contributors
-# Authors: Marco Garten, Axel Huebl, CHad Mitchell
+# Copyright 2022-2025 ImpactX contributors
+# Authors: Chad Mitchell
 # License: BSD-3-Clause-LBNL
 #
 # -*- coding: utf-8 -*-