diff --git a/scipost_django/scipost/tests/test_services.py b/scipost_django/scipost/tests/test_services.py
index 38259224c61905e0772295cb6eb089b8a335e4a3..34866a88335b494cf894dcb46d1638b9f5e9a43f 100644
--- a/scipost_django/scipost/tests/test_services.py
+++ b/scipost_django/scipost/tests/test_services.py
@@ -22,9 +22,9 @@ class ArxivCallerTest(TestCase):
         correct_data = {
             "arxiv_link": "https://arxiv.org/abs/1612.07611v1",
             "author_list": "Roman Krčmár, Andrej Gendiar, Tomotoshi Nishino",
-            "abstract": "The Berezinskii-Kosterlitz-Thouless (BKT) transitions of the six-state clock\nmodel on the square lattice are investigated by means of the corner-transfer\nmatrix renormalization group method. The classical analogue of the entanglement\nentropy $S( L, T )$ is calculated for $L$ by $L$ square system up to $L = 129$,\nas a function of temperature $T$. The entropy has a peak at $T = T^{*}_{~}( L\n)$, where the temperature depends on both $L$ and boundary conditions. Applying\nthe finite-size scaling to $T^{*}_{~}( L )$ and assuming the presence of BKT\ntransitions, the transition temperature is estimated to be $T_1^{~} = 0.70$ and\n$T_2^{~} = 0.88$. The obtained results agree with previous analyses. It should\nbe noted that no thermodynamic function is used in this study.",
-            "pub_abstract": "The Berezinskii-Kosterlitz-Thouless (BKT) transitions of the six-state clock\nmodel on the square lattice are investigated by means of the corner-transfer\nmatrix renormalization group method. The classical analogue of the entanglement\nentropy $S( L, T )$ is calculated for $L$ by $L$ square system up to $L = 129$,\nas a function of temperature $T$. The entropy has a peak at $T = T^{*}_{~}( L\n)$, where the temperature depends on both $L$ and boundary conditions. Applying\nthe finite-size scaling to $T^{*}_{~}( L )$ and assuming the presence of BKT\ntransitions, the transition temperature is estimated to be $T_1^{~} = 0.70$ and\n$T_2^{~} = 0.88$. The obtained results agree with previous analyses. It should\nbe noted that no thermodynamic function is used in this study.",
-            "title": "Phase transition of the six-state clock model observed from the\n  entanglement entropy",
+            "abstract": "The Berezinskii-Kosterlitz-Thouless (BKT) transitions of the six-state clock model on the square lattice are investigated by means of the corner-transfer matrix renormalization group method. The classical analogue of the entanglement entropy $S( L, T )$ is calculated for $L$ by $L$ square system up to $L = 129$, as a function of temperature $T$. The entropy has a peak at $T = T^{*}_{~}( L )$, where the temperature depends on both $L$ and boundary conditions. Applying the finite-size scaling to $T^{*}_{~}( L )$ and assuming the presence of BKT transitions, the transition temperature is estimated to be $T_1^{~} = 0.70$ and $T_2^{~} = 0.88$. The obtained results agree with previous analyses. It should be noted that no thermodynamic function is used in this study.",
+            "pub_abstract": "The Berezinskii-Kosterlitz-Thouless (BKT) transitions of the six-state clock model on the square lattice are investigated by means of the corner-transfer matrix renormalization group method. The classical analogue of the entanglement entropy $S( L, T )$ is calculated for $L$ by $L$ square system up to $L = 129$, as a function of temperature $T$. The entropy has a peak at $T = T^{*}_{~}( L )$, where the temperature depends on both $L$ and boundary conditions. Applying the finite-size scaling to $T^{*}_{~}( L )$ and assuming the presence of BKT transitions, the transition temperature is estimated to be $T_1^{~} = 0.70$ and $T_2^{~} = 0.88$. The obtained results agree with previous analyses. It should be noted that no thermodynamic function is used in this study.",
+            "title": "Phase transition of the six-state clock model observed from the entanglement entropy",
             "preprint_link": "https://arxiv.org/abs/1612.07611v1",
             "pub_date": datetime.date(2016, 12, 22),
         }
@@ -38,9 +38,9 @@ class ArxivCallerTest(TestCase):
             "arxiv_link": "https://arxiv.org/abs/cond-mat/0612480v2",
             "pub_date": datetime.date(2006, 12, 19),
             "author_list": "Kouji Ueda, Chenglong Jin, Naokazu Shibata, Yasuhiro Hieida, Tomotoshi Nishino",
-            "abstract": "A kind of least action principle is introduced for the discrete time\nevolution of one-dimensional quantum lattice models. Based on this principle,\nwe obtain an optimal condition for the matrix product states on succeeding time\nslices generated by the real-time density matrix renormalization group method.\nThis optimization can also be applied to classical simulations of quantum\ncircuits. We discuss the time reversal symmetry in the fully optimized MPS.",
-            "pub_abstract": "A kind of least action principle is introduced for the discrete time\nevolution of one-dimensional quantum lattice models. Based on this principle,\nwe obtain an optimal condition for the matrix product states on succeeding time\nslices generated by the real-time density matrix renormalization group method.\nThis optimization can also be applied to classical simulations of quantum\ncircuits. We discuss the time reversal symmetry in the fully optimized MPS.",
-            "title": "Least Action Principle for the Real-Time Density Matrix Renormalization\n  Group",
+            "abstract": "A kind of least action principle is introduced for the discrete time evolution of one-dimensional quantum lattice models. Based on this principle, we obtain an optimal condition for the matrix product states on succeeding time slices generated by the real-time density matrix renormalization group method. This optimization can also be applied to classical simulations of quantum circuits. We discuss the time reversal symmetry in the fully optimized MPS.",
+            "pub_abstract": "A kind of least action principle is introduced for the discrete time evolution of one-dimensional quantum lattice models. Based on this principle, we obtain an optimal condition for the matrix product states on succeeding time slices generated by the real-time density matrix renormalization group method. This optimization can also be applied to classical simulations of quantum circuits. We discuss the time reversal symmetry in the fully optimized MPS.",
+            "title": "Least Action Principle for the Real-Time Density Matrix Renormalization Group",
             "preprint_link": "https://arxiv.org/abs/cond-mat/0612480v2",
         }
         del caller.data["preprint_server"]  # Remove server key before comparison
diff --git a/scipost_django/scipost/tests/test_views.py b/scipost_django/scipost/tests/test_views.py
index 2e5f2b550217f530174eb48d45e6e84e625e36c3..b9d0070ccbee6c4c276e53aea878b941da931368 100644
--- a/scipost_django/scipost/tests/test_views.py
+++ b/scipost_django/scipost/tests/test_views.py
@@ -102,18 +102,3 @@ class VetCommentaryRequestsTest(TestCase):
         UnvettedCommentaryFactory()
         response = self.client.get(self.view_url)
         self.assertTrue(type(response.context["commentary_to_vet"]) is Commentary)
-
-
-class CommentaryDetailTest(TestCase):
-    def setUp(self):
-        add_groups_and_permissions()
-        self.client = Client()
-        self.commentary = UnpublishedCommentaryFactory()
-        self.target = reverse(
-            "commentaries:commentary",
-            kwargs={"arxiv_or_DOI_string": self.commentary.arxiv_or_DOI_string},
-        )
-
-    def test_status_code_200(self):
-        response = self.client.get(self.target)
-        self.assertEqual(response.status_code, 200)