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doc/Projects/2026/Project1/html/._Project1-bs000.html

Lines changed: 21 additions & 17 deletions
Original file line numberDiff line numberDiff line change
@@ -37,12 +37,12 @@
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<!-- tocinfo
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{'highest level': 1,
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'sections': [('Project suggestion', 1, None, 'project-suggestion'),
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('Part a) (score 10pt)', 2, None, 'part-a-score-10pt'),
40+
('Part a) (score 15pt)', 2, None, 'part-a-score-15pt'),
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('Part b) (score 10pt)', 2, None, 'part-b-score-10pt'),
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('Part c) (score 10pt)', 2, None, 'part-c-score-10pt'),
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('Part d) (score 15pt)', 2, None, 'part-d-score-15pt'),
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('Part e) (score 15 pt)', 2, None, 'part-e-score-15-pt'),
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('Part f) (score 20 pt)', 2, None, 'part-f-score-20-pt'),
45+
('Part f) (score 15 pt)', 2, None, 'part-f-score-15-pt'),
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('Part g) (score 20 pt)', 2, None, 'part-g-score-20-pt'),
4747
('Introduction to numerical projects',
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2,
@@ -87,12 +87,12 @@
8787
<a href="#" class="dropdown-toggle" data-toggle="dropdown">Contents <b class="caret"></b></a>
8888
<ul class="dropdown-menu">
8989
<!-- navigation toc: --> <li><a href="#project-suggestion" style="font-size: 80%;"><b>Project suggestion</b></a></li>
90-
<!-- navigation toc: --> <li><a href="#part-a-score-10pt" style="font-size: 80%;">&nbsp;&nbsp;&nbsp;Part a) (score 10pt)</a></li>
90+
<!-- navigation toc: --> <li><a href="#part-a-score-15pt" style="font-size: 80%;">&nbsp;&nbsp;&nbsp;Part a) (score 15pt)</a></li>
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<!-- navigation toc: --> <li><a href="#part-b-score-10pt" style="font-size: 80%;">&nbsp;&nbsp;&nbsp;Part b) (score 10pt)</a></li>
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<!-- navigation toc: --> <li><a href="#part-c-score-10pt" style="font-size: 80%;">&nbsp;&nbsp;&nbsp;Part c) (score 10pt)</a></li>
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<!-- navigation toc: --> <li><a href="#part-d-score-15pt" style="font-size: 80%;">&nbsp;&nbsp;&nbsp;Part d) (score 15pt)</a></li>
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<!-- navigation toc: --> <li><a href="#part-e-score-15-pt" style="font-size: 80%;">&nbsp;&nbsp;&nbsp;Part e) (score 15 pt)</a></li>
95-
<!-- navigation toc: --> <li><a href="#part-f-score-20-pt" style="font-size: 80%;">&nbsp;&nbsp;&nbsp;Part f) (score 20 pt)</a></li>
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<!-- navigation toc: --> <li><a href="#part-f-score-15-pt" style="font-size: 80%;">&nbsp;&nbsp;&nbsp;Part f) (score 15 pt)</a></li>
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<!-- navigation toc: --> <li><a href="#part-g-score-20-pt" style="font-size: 80%;">&nbsp;&nbsp;&nbsp;Part g) (score 20 pt)</a></li>
9797
<!-- navigation toc: --> <li><a href="#introduction-to-numerical-projects" style="font-size: 80%;">&nbsp;&nbsp;&nbsp;Introduction to numerical projects</a></li>
9898
<!-- navigation toc: --> <li><a href="#format-for-electronic-delivery-of-report-and-programs" style="font-size: 80%;">&nbsp;&nbsp;&nbsp;Format for electronic delivery of report and programs</a></li>
@@ -131,9 +131,7 @@ <h1 id="project-suggestion" class="anchor">Project suggestion </h1>
131131
The total score is 100 points. You can answer each exercise in a sequential way or write a scientific report. Each exercise is given a final score.
132132
If you plan to write a report, you could use the article in the Physical Review C, volume 106, see <a href="https://journals.aps.org/prc/pdf/10.1103/PhysRevC.106.024319" target="_self"><tt>https://journals.aps.org/prc/pdf/10.1103/PhysRevC.106.024319</tt></a> as a template for your report.
133133
</p>
134-
135-
<p><b>Note:</b> This is prelimary version, changes will come and the final version is availbale from February 2.</p>
136-
<h2 id="part-a-score-10pt" class="anchor">Part a) (score 10pt) </h2>
134+
<h2 id="part-a-score-15pt" class="anchor">Part a) (score 15pt) </h2>
137135

138136
<p>Write a function which sets up a one-qubit basis and apply the various
139137
Pauli matrices to these basis states. Apply the Hadamard and Phase
@@ -146,7 +144,12 @@ <h2 id="part-a-score-10pt" class="anchor">Part a) (score 10pt) </h2>
146144
which should be discussed and presented.
147145
</p>
148146

149-
<p>Compare your code with the results obtained using for example software like <b>Qiskit</b>.</p>
147+
<p>For the Bell states (one of your choice), you should also write a code
148+
which traces out the density matrix for one subsystem and calculate
149+
the von Neumann entropy and discuss the results.
150+
</p>
151+
152+
<!-- You can compare your code with the results obtained using for example software like <b>Qiskit</b>. -->
150153
<h2 id="part-b-score-10pt" class="anchor">Part b) (score 10pt) </h2>
151154

152155
<p>We define a symmetric matrix \( H\in {\mathbb{R}}^{2\times 2} \)</p>
@@ -222,7 +225,7 @@ <h2 id="part-b-score-10pt" class="anchor">Part b) (score 10pt) </h2>
222225
\( \vert 0 \rangle \) component of more than \( 90\% \). The character of the
223226
eigenvectors has therefore been interchanged when passing \( z=2/3 \). The
224227
value of the parameter \( V_{12} \) represents the strength of the coupling
225-
between the two states..
228+
between the two states.
226229
</p>
227230

228231
<p>Solve <b>by standard eigenvalue solvers</b> (either numerically or analytically) the above eigenvalue problem.
@@ -235,9 +238,9 @@ <h2 id="part-c-score-10pt" class="anchor">Part c) (score 10pt) </h2>
235238
<p>Implement now the variational quantum eigensolver (VQE) for the above
236239
Hamiltonian and set up the circuit(s) which is(are) needed in order to find
237240
the eigenvalues of this system. Discuss the results and compare these
238-
with those from part b). Feel free to use either <b>Qiskit</b> or your own
239-
code (based on the setup from part a)) or both approaches. Discuss
240-
your results.
241+
with those from part b). You have to write your own code for the VQE but you can compare your code
242+
with either <b>Qiskit</b> or other software libraries like <b>Pennylane</b> or other.
243+
Discuss your results.
241244
</p>
242245
<h2 id="part-d-score-15pt" class="anchor">Part d) (score 15pt) </h2>
243246

@@ -336,7 +339,7 @@ <h2 id="part-d-score-15pt" class="anchor">Part d) (score 15pt) </h2>
336339
$$
337340

338341
<p>The density matrices for these subsets can be used to compute the
339-
so-called von Neumann entropy, which is one of the possible measures
342+
von Neumann entropy discussed in exercise a), which is one of the possible measures
340343
of entanglement. A pure state has entropy equal zero while entangled
341344
state have an entropy larger than zero. The von-Neumann entropy is
342345
defined as
@@ -396,11 +399,12 @@ <h2 id="part-e-score-15-pt" class="anchor">Part e) (score 15 pt) </h2>
396399

397400
<p>Compute now the eigenvalues of this system using the VQE method and
398401
set up the circuits needed to find the lowest state. Compare these
399-
results with those from the previous part. Feel free again to either
400-
use your own code for the circuit and your VQE code or use the
401-
functionality of <a href="https://qiskit.org/" target="_self">Qiskit</a>, or both.
402+
results with those from the previous part.
403+
You have to write your own code for the VQE but you can compare your code
404+
with either <b>Qiskit</b> or other software libraries like <b>Pennylane</b> or other.
405+
Discuss your results.
402406
</p>
403-
<h2 id="part-f-score-20-pt" class="anchor">Part f) (score 20 pt) </h2>
407+
<h2 id="part-f-score-15-pt" class="anchor">Part f) (score 15 pt) </h2>
404408

405409
<p>We introduce now the Lipkin Hamiltonian and study this for the
406410
\( 3\times 3 \) matrix case with total spin \( J=1 \) and the \( 5\times 5 \)

doc/Projects/2026/Project1/html/Project1-bs.html

Lines changed: 21 additions & 17 deletions
Original file line numberDiff line numberDiff line change
@@ -37,12 +37,12 @@
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<!-- tocinfo
3838
{'highest level': 1,
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'sections': [('Project suggestion', 1, None, 'project-suggestion'),
40-
('Part a) (score 10pt)', 2, None, 'part-a-score-10pt'),
40+
('Part a) (score 15pt)', 2, None, 'part-a-score-15pt'),
4141
('Part b) (score 10pt)', 2, None, 'part-b-score-10pt'),
4242
('Part c) (score 10pt)', 2, None, 'part-c-score-10pt'),
4343
('Part d) (score 15pt)', 2, None, 'part-d-score-15pt'),
4444
('Part e) (score 15 pt)', 2, None, 'part-e-score-15-pt'),
45-
('Part f) (score 20 pt)', 2, None, 'part-f-score-20-pt'),
45+
('Part f) (score 15 pt)', 2, None, 'part-f-score-15-pt'),
4646
('Part g) (score 20 pt)', 2, None, 'part-g-score-20-pt'),
4747
('Introduction to numerical projects',
4848
2,
@@ -87,12 +87,12 @@
8787
<a href="#" class="dropdown-toggle" data-toggle="dropdown">Contents <b class="caret"></b></a>
8888
<ul class="dropdown-menu">
8989
<!-- navigation toc: --> <li><a href="#project-suggestion" style="font-size: 80%;"><b>Project suggestion</b></a></li>
90-
<!-- navigation toc: --> <li><a href="#part-a-score-10pt" style="font-size: 80%;">&nbsp;&nbsp;&nbsp;Part a) (score 10pt)</a></li>
90+
<!-- navigation toc: --> <li><a href="#part-a-score-15pt" style="font-size: 80%;">&nbsp;&nbsp;&nbsp;Part a) (score 15pt)</a></li>
9191
<!-- navigation toc: --> <li><a href="#part-b-score-10pt" style="font-size: 80%;">&nbsp;&nbsp;&nbsp;Part b) (score 10pt)</a></li>
9292
<!-- navigation toc: --> <li><a href="#part-c-score-10pt" style="font-size: 80%;">&nbsp;&nbsp;&nbsp;Part c) (score 10pt)</a></li>
9393
<!-- navigation toc: --> <li><a href="#part-d-score-15pt" style="font-size: 80%;">&nbsp;&nbsp;&nbsp;Part d) (score 15pt)</a></li>
9494
<!-- navigation toc: --> <li><a href="#part-e-score-15-pt" style="font-size: 80%;">&nbsp;&nbsp;&nbsp;Part e) (score 15 pt)</a></li>
95-
<!-- navigation toc: --> <li><a href="#part-f-score-20-pt" style="font-size: 80%;">&nbsp;&nbsp;&nbsp;Part f) (score 20 pt)</a></li>
95+
<!-- navigation toc: --> <li><a href="#part-f-score-15-pt" style="font-size: 80%;">&nbsp;&nbsp;&nbsp;Part f) (score 15 pt)</a></li>
9696
<!-- navigation toc: --> <li><a href="#part-g-score-20-pt" style="font-size: 80%;">&nbsp;&nbsp;&nbsp;Part g) (score 20 pt)</a></li>
9797
<!-- navigation toc: --> <li><a href="#introduction-to-numerical-projects" style="font-size: 80%;">&nbsp;&nbsp;&nbsp;Introduction to numerical projects</a></li>
9898
<!-- navigation toc: --> <li><a href="#format-for-electronic-delivery-of-report-and-programs" style="font-size: 80%;">&nbsp;&nbsp;&nbsp;Format for electronic delivery of report and programs</a></li>
@@ -131,9 +131,7 @@ <h1 id="project-suggestion" class="anchor">Project suggestion </h1>
131131
The total score is 100 points. You can answer each exercise in a sequential way or write a scientific report. Each exercise is given a final score.
132132
If you plan to write a report, you could use the article in the Physical Review C, volume 106, see <a href="https://journals.aps.org/prc/pdf/10.1103/PhysRevC.106.024319" target="_self"><tt>https://journals.aps.org/prc/pdf/10.1103/PhysRevC.106.024319</tt></a> as a template for your report.
133133
</p>
134-
135-
<p><b>Note:</b> This is prelimary version, changes will come and the final version is availbale from February 2.</p>
136-
<h2 id="part-a-score-10pt" class="anchor">Part a) (score 10pt) </h2>
134+
<h2 id="part-a-score-15pt" class="anchor">Part a) (score 15pt) </h2>
137135

138136
<p>Write a function which sets up a one-qubit basis and apply the various
139137
Pauli matrices to these basis states. Apply the Hadamard and Phase
@@ -146,7 +144,12 @@ <h2 id="part-a-score-10pt" class="anchor">Part a) (score 10pt) </h2>
146144
which should be discussed and presented.
147145
</p>
148146

149-
<p>Compare your code with the results obtained using for example software like <b>Qiskit</b>.</p>
147+
<p>For the Bell states (one of your choice), you should also write a code
148+
which traces out the density matrix for one subsystem and calculate
149+
the von Neumann entropy and discuss the results.
150+
</p>
151+
152+
<!-- You can compare your code with the results obtained using for example software like <b>Qiskit</b>. -->
150153
<h2 id="part-b-score-10pt" class="anchor">Part b) (score 10pt) </h2>
151154

152155
<p>We define a symmetric matrix \( H\in {\mathbb{R}}^{2\times 2} \)</p>
@@ -222,7 +225,7 @@ <h2 id="part-b-score-10pt" class="anchor">Part b) (score 10pt) </h2>
222225
\( \vert 0 \rangle \) component of more than \( 90\% \). The character of the
223226
eigenvectors has therefore been interchanged when passing \( z=2/3 \). The
224227
value of the parameter \( V_{12} \) represents the strength of the coupling
225-
between the two states..
228+
between the two states.
226229
</p>
227230

228231
<p>Solve <b>by standard eigenvalue solvers</b> (either numerically or analytically) the above eigenvalue problem.
@@ -235,9 +238,9 @@ <h2 id="part-c-score-10pt" class="anchor">Part c) (score 10pt) </h2>
235238
<p>Implement now the variational quantum eigensolver (VQE) for the above
236239
Hamiltonian and set up the circuit(s) which is(are) needed in order to find
237240
the eigenvalues of this system. Discuss the results and compare these
238-
with those from part b). Feel free to use either <b>Qiskit</b> or your own
239-
code (based on the setup from part a)) or both approaches. Discuss
240-
your results.
241+
with those from part b). You have to write your own code for the VQE but you can compare your code
242+
with either <b>Qiskit</b> or other software libraries like <b>Pennylane</b> or other.
243+
Discuss your results.
241244
</p>
242245
<h2 id="part-d-score-15pt" class="anchor">Part d) (score 15pt) </h2>
243246

@@ -336,7 +339,7 @@ <h2 id="part-d-score-15pt" class="anchor">Part d) (score 15pt) </h2>
336339
$$
337340

338341
<p>The density matrices for these subsets can be used to compute the
339-
so-called von Neumann entropy, which is one of the possible measures
342+
von Neumann entropy discussed in exercise a), which is one of the possible measures
340343
of entanglement. A pure state has entropy equal zero while entangled
341344
state have an entropy larger than zero. The von-Neumann entropy is
342345
defined as
@@ -396,11 +399,12 @@ <h2 id="part-e-score-15-pt" class="anchor">Part e) (score 15 pt) </h2>
396399

397400
<p>Compute now the eigenvalues of this system using the VQE method and
398401
set up the circuits needed to find the lowest state. Compare these
399-
results with those from the previous part. Feel free again to either
400-
use your own code for the circuit and your VQE code or use the
401-
functionality of <a href="https://qiskit.org/" target="_self">Qiskit</a>, or both.
402+
results with those from the previous part.
403+
You have to write your own code for the VQE but you can compare your code
404+
with either <b>Qiskit</b> or other software libraries like <b>Pennylane</b> or other.
405+
Discuss your results.
402406
</p>
403-
<h2 id="part-f-score-20-pt" class="anchor">Part f) (score 20 pt) </h2>
407+
<h2 id="part-f-score-15-pt" class="anchor">Part f) (score 15 pt) </h2>
404408

405409
<p>We introduce now the Lipkin Hamiltonian and study this for the
406410
\( 3\times 3 \) matrix case with total spin \( J=1 \) and the \( 5\times 5 \)

doc/Projects/2026/Project1/html/Project1.html

Lines changed: 19 additions & 15 deletions
Original file line numberDiff line numberDiff line change
@@ -115,12 +115,12 @@
115115
<!-- tocinfo
116116
{'highest level': 1,
117117
'sections': [('Project suggestion', 1, None, 'project-suggestion'),
118-
('Part a) (score 10pt)', 2, None, 'part-a-score-10pt'),
118+
('Part a) (score 15pt)', 2, None, 'part-a-score-15pt'),
119119
('Part b) (score 10pt)', 2, None, 'part-b-score-10pt'),
120120
('Part c) (score 10pt)', 2, None, 'part-c-score-10pt'),
121121
('Part d) (score 15pt)', 2, None, 'part-d-score-15pt'),
122122
('Part e) (score 15 pt)', 2, None, 'part-e-score-15-pt'),
123-
('Part f) (score 20 pt)', 2, None, 'part-f-score-20-pt'),
123+
('Part f) (score 15 pt)', 2, None, 'part-f-score-15-pt'),
124124
('Part g) (score 20 pt)', 2, None, 'part-g-score-20-pt'),
125125
('Introduction to numerical projects',
126126
2,
@@ -170,9 +170,7 @@ <h1 id="project-suggestion">Project suggestion </h1>
170170
The total score is 100 points. You can answer each exercise in a sequential way or write a scientific report. Each exercise is given a final score.
171171
If you plan to write a report, you could use the article in the Physical Review C, volume 106, see <a href="https://journals.aps.org/prc/pdf/10.1103/PhysRevC.106.024319" target="_blank"><tt>https://journals.aps.org/prc/pdf/10.1103/PhysRevC.106.024319</tt></a> as a template for your report.
172172
</p>
173-
174-
<p><b>Note:</b> This is prelimary version, changes will come and the final version is availbale from February 2.</p>
175-
<h2 id="part-a-score-10pt">Part a) (score 10pt) </h2>
173+
<h2 id="part-a-score-15pt">Part a) (score 15pt) </h2>
176174

177175
<p>Write a function which sets up a one-qubit basis and apply the various
178176
Pauli matrices to these basis states. Apply the Hadamard and Phase
@@ -185,7 +183,12 @@ <h2 id="part-a-score-10pt">Part a) (score 10pt) </h2>
185183
which should be discussed and presented.
186184
</p>
187185

188-
<p>Compare your code with the results obtained using for example software like <b>Qiskit</b>.</p>
186+
<p>For the Bell states (one of your choice), you should also write a code
187+
which traces out the density matrix for one subsystem and calculate
188+
the von Neumann entropy and discuss the results.
189+
</p>
190+
191+
<!-- You can compare your code with the results obtained using for example software like <b>Qiskit</b>. -->
189192
<h2 id="part-b-score-10pt">Part b) (score 10pt) </h2>
190193

191194
<p>We define a symmetric matrix \( H\in {\mathbb{R}}^{2\times 2} \)</p>
@@ -261,7 +264,7 @@ <h2 id="part-b-score-10pt">Part b) (score 10pt) </h2>
261264
\( \vert 0 \rangle \) component of more than \( 90\% \). The character of the
262265
eigenvectors has therefore been interchanged when passing \( z=2/3 \). The
263266
value of the parameter \( V_{12} \) represents the strength of the coupling
264-
between the two states..
267+
between the two states.
265268
</p>
266269

267270
<p>Solve <b>by standard eigenvalue solvers</b> (either numerically or analytically) the above eigenvalue problem.
@@ -274,9 +277,9 @@ <h2 id="part-c-score-10pt">Part c) (score 10pt) </h2>
274277
<p>Implement now the variational quantum eigensolver (VQE) for the above
275278
Hamiltonian and set up the circuit(s) which is(are) needed in order to find
276279
the eigenvalues of this system. Discuss the results and compare these
277-
with those from part b). Feel free to use either <b>Qiskit</b> or your own
278-
code (based on the setup from part a)) or both approaches. Discuss
279-
your results.
280+
with those from part b). You have to write your own code for the VQE but you can compare your code
281+
with either <b>Qiskit</b> or other software libraries like <b>Pennylane</b> or other.
282+
Discuss your results.
280283
</p>
281284
<h2 id="part-d-score-15pt">Part d) (score 15pt) </h2>
282285

@@ -375,7 +378,7 @@ <h2 id="part-d-score-15pt">Part d) (score 15pt) </h2>
375378
$$
376379

377380
<p>The density matrices for these subsets can be used to compute the
378-
so-called von Neumann entropy, which is one of the possible measures
381+
von Neumann entropy discussed in exercise a), which is one of the possible measures
379382
of entanglement. A pure state has entropy equal zero while entangled
380383
state have an entropy larger than zero. The von-Neumann entropy is
381384
defined as
@@ -435,11 +438,12 @@ <h2 id="part-e-score-15-pt">Part e) (score 15 pt) </h2>
435438

436439
<p>Compute now the eigenvalues of this system using the VQE method and
437440
set up the circuits needed to find the lowest state. Compare these
438-
results with those from the previous part. Feel free again to either
439-
use your own code for the circuit and your VQE code or use the
440-
functionality of <a href="https://qiskit.org/" target="_blank">Qiskit</a>, or both.
441+
results with those from the previous part.
442+
You have to write your own code for the VQE but you can compare your code
443+
with either <b>Qiskit</b> or other software libraries like <b>Pennylane</b> or other.
444+
Discuss your results.
441445
</p>
442-
<h2 id="part-f-score-20-pt">Part f) (score 20 pt) </h2>
446+
<h2 id="part-f-score-15-pt">Part f) (score 15 pt) </h2>
443447

444448
<p>We introduce now the Lipkin Hamiltonian and study this for the
445449
\( 3\times 3 \) matrix case with total spin \( J=1 \) and the \( 5\times 5 \)

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