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- [
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- {
3
- "category": "theory",
4
- "question": "Ionospheric refraction increases the zenith angle of incoming radio waves in the frequency range relevant to EoR as they pass through the a homogeneous F-layer of the ionosphere.",
5
- "choices": {
6
- "A": "yes",
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- "B": "no",
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- "C": "dunno"
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- },
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- "answer": {
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- "type": "string",
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- "enum": [
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- "A",
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- "B",
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- "C"
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- ],
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- "description": "Your selected answer (A, B, or C)"
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- },
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- "ideal": "B",
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- "task": 5,
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- "tolerance": 0,
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- "N": 0,
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- "score": 0,
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- "reference": "https://academic.oup.com/mnras/article/503/1/344/6145010",
25
- "reason": "The F-layer refraction bends the signal towards the zenith as it passes through the F-layer, decreasing the zenith angle."
26
- },
27
- {
28
- "category": "theory",
29
- "question": "In the absence of X-ray heating and ionization, The 21-cm signal during the cosmic dawn or EoR is sensitive to the details of the IMF and can probe the typical mass of stars if it is dominated by stars heavier than 20 solar masses.",
30
- "choices": {
31
- "A": "yes",
32
- "B": "no",
33
- "C": "dunno"
34
- },
35
- "answer": {
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- "type": "string",
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- "enum": [
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- "A",
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- "B",
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- "C"
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- ],
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- "description": "Your selected answer (A, B, or C)"
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- },
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- "ideal": "B",
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- "task": 5,
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- "tolerance": 0,
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- "N": 0,
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- "score": 0,
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- "reference": "https://academic.oup.com/mnras/article/516/1/841/6648845?login=true",
50
- "reason": ""
51
- },
52
- {
53
- "category": "theory",
54
- "question": "Global 21-cm absorption feature during cosmic dawn/ EoR becomes deeper with increasing x-ray emissivity.",
55
- "choices": {
56
- "A": "yes",
57
- "B": "no",
58
- "C": "dunno"
59
- },
60
- "answer": {
61
- "type": "string",
62
- "enum": [
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- "A",
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- "B",
65
- "C"
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- ],
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- "description": "Your selected answer (A, B, or C)"
68
- },
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- "ideal": "B",
70
- "task": 5,
71
- "tolerance": 0,
72
- "N": 0,
73
- "score": 0,
74
- "reference": "https://iopscience.iop.org/article/10.1088/0034-4885/75/8/086901",
75
- "reason": "Increasing x-ray emissivity heats IGM, making the difference to the 21-cm spin temperature smaller and the absorption feature shallower."
76
- },
77
- {
78
- "category": "theory",
79
- "question": "Global 21-cm absorption feature during cosmic dawn/ EoR becomes deeper with increasing lyman-alpha emissivity.",
80
- "choices": {
81
- "A": "yes",
82
- "B": "no",
83
- "C": "dunno"
84
- },
85
- "answer": {
86
- "type": "string",
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- "enum": [
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- "A",
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- "B",
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- "C"
91
- ],
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- "description": "Your selected answer (A, B, or C)"
93
- },
94
- "ideal": "A",
95
- "task": 5,
96
- "tolerance": 0,
97
- "N": 0,
98
- "score": 0,
99
- "reference": "https://iopscience.iop.org/article/10.1088/0034-4885/75/8/086901",
100
- "reason": "Increased Lyman-alpha emissivity enhances the Wouthuysen-Field effect, coupling the spin temperature to the cold gas, deepening the absorption feature."
101
- },
102
- {
103
- "category": "experiment",
104
- "question": "The REACH global 21-cm experiment uses polynomials to fit the astrophysical foregrounds",
105
- "choices": {
106
- "A": "yes",
107
- "B": "no",
108
- "C": "dunno"
109
- },
110
- "answer": {
111
- "type": "string",
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- "enum": [
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- "A",
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- "B",
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- "C"
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- ],
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- "description": "Your selected answer (A, B, or C)"
118
- },
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- "ideal": "B",
120
- "task": 5,
121
- "tolerance": 0,
122
- "N": 0,
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- "score": 0,
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- "reference": "https://academic.oup.com/mnras/article/506/2/2041/6307526?login=true",
125
- "reason": "It uses a sophisticated sky division model based on spectral index."
126
- },
127
- {
128
- "category": "theory",
129
- "question": "In 21-cm cosmology, which process strongly couples the spin and kinetic temperatures?",
130
- "choices": {
131
- "A": "Compton scattering",
132
- "B": "Wouthuysen-Field effect",
133
- "C": "collisional coupling"
134
- },
135
- "answer": {
136
- "type": "string",
137
- "enum": [
138
- "A",
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- "B",
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- "C"
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- ],
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- "description": "Your selected answer (A, B, or C)"
143
- },
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- "ideal": "B",
145
- "task": 5,
146
- "tolerance": 0,
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- "N": 0,
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- "score": 0,
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- "reference": "https://ieeexplore.ieee.org/document/4065250",
150
- "reason": ""
151
- },
152
- {
153
- "category": "theory",
154
- "question": "At redshift 300, the gas kinetic temperature decreases more slowly than the radio background temperature.",
155
- "choices": {
156
- "A": "yes",
157
- "B": "no",
158
- "C": "dunno"
159
- },
160
- "answer": {
161
- "type": "string",
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- "enum": [
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- "A",
164
- "B",
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- "C"
166
- ],
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- "description": "Your selected answer (A, B, or C)"
168
- },
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- "ideal": "B",
170
- "task": 5,
171
- "tolerance": 0,
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- "N": 0,
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- "score": 0,
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- "reference": "",
175
- "reason": "The gas kinetic temperature decreases adiabatically as (1+z)^2, while the radio background temperature decreases as (1+z); it decreases faster."
176
- },
177
- {
178
- "category": "theory",
179
- "question": "What is the dominant heating mechanism until around redshift 150?",
180
- "choices": {
181
- "A": "Compton scattering",
182
- "B": "Wouthuysen-Field effect",
183
- "C": "X-ray heating"
184
- },
185
- "answer": {
186
- "type": "string",
187
- "enum": [
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- "A",
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- "B",
190
- "C"
191
- ],
192
- "description": "Your selected answer (A, B, or C)"
193
- },
194
- "ideal": "A",
195
- "task": 5,
196
- "tolerance": 0,
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- "N": 0,
198
- "score": 0,
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- "reference": "https://iopscience.iop.org/article/10.1088/0034-4885/75/8/086901",
200
- "reason": ""
201
- },
202
- {
203
- "category": "theory",
204
- "question": "At which redshift does Compton heating become ineffective at coupling the gas kinetic temperature to the radio background temperature?",
205
- "choices": {
206
- "A": "50",
207
- "B": "100",
208
- "C": "150"
209
- },
210
- "answer": {
211
- "type": "string",
212
- "enum": [
213
- "A",
214
- "B",
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- "C"
216
- ],
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- "description": "Your selected answer (A, B, or C)"
218
- },
219
- "ideal": "C",
220
- "task": 5,
221
- "tolerance": 0,
222
- "N": 0,
223
- "score": 0,
224
- "reference": "https://iopscience.iop.org/article/10.1088/0034-4885/75/8/086901",
225
- "reason": ""
226
- },
227
-
228
- {
229
- "category": "theory",
230
- "question": "What is the primary astrophysical mechanism that heats the intergalactic medium (IGM) during the cosmic dawn?",
231
- "choices": {
232
- "A": "X-ray heating",
233
- "B": "Lyman-alpha heating",
234
- "C": "Cosmic ray heating"
235
- },
236
- "answer": {
237
- "type": "string",
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- "enum": [
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- "A",
240
- "B",
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- "C"
242
- ],
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- "description": "Your selected answer (A, B, or C)"
244
- },
245
- "ideal": "A",
246
- "task": 5,
247
- "tolerance": 0,
248
- "N": 0,
249
- "score": 0,
250
- "reference": "https://iopscience.iop.org/article/10.1086/323691",
251
- "reason": ""
252
- },
253
- {
254
- "category": "theory",
255
- "question": "It is generally assumed that the Universe was reionised by UV photons, but X-rays could potentially fully reionise the Universe.",
256
- "choices": {
257
- "A": "yes",
258
- "B": "no",
259
- "C": "dunno"
260
- },
261
- "answer": {
262
- "type": "string",
263
- "enum": [
264
- "A",
265
- "B",
266
- "C"
267
- ],
268
- "description": "Your selected answer (A, B, or C)"
269
- },
270
- "ideal": "B",
271
- "task": 5,
272
- "tolerance": 0,
273
- "N": 0,
274
- "score": 0,
275
- "reference": "https://academic.oup.com/mnras/article/426/2/1349/974573",
276
- "reason": "Chandra observations place limits on this contribution of X-ray to reionisation."
277
- },
278
- {
279
- "category": "theory",
280
- "question": "The 21-cm signal is observable in emission during the early stages of reionisation before significant heating.",
281
- "choices": {
282
- "A": "yes",
283
- "B": "no",
284
- "C": "dunno"
285
- },
286
- "answer": {
287
- "type": "string",
288
- "enum": [
289
- "A",
290
- "B",
291
- "C"
292
- ],
293
- "description": "Your selected answer (A, B, or C)"
294
- },
295
- "ideal": "B",
296
- "task": 5,
297
- "tolerance": 0,
298
- "N": 0,
299
- "score": 0,
300
- "reference": "https://iopscience.iop.org/article/10.1088/0034-4885/75/8/086901",
301
- "reason": "Before significant heating, the spin temperature is coupled to the CMB temperature, making the 21-cm signal observable in absorption."
302
- },
303
- {
304
- "category": "theory",
305
- "question": "Which radiation background is responsible for the coupling of the spin temperature before reionisation starts?",
306
- "choices": {
307
- "A": "cosmic microwave background",
308
- "B": "X-ray radiation",
309
- "C": "Lyman-alpha radiation"
310
- },
311
- "answer": {
312
- "type": "string",
313
- "enum": [
314
- "A",
315
- "B",
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- "C"
317
- ],
318
- "description": "Your selected answer (A, B, or C)"
319
- },
320
- "ideal": "C",
321
- "task": 5,
322
- "tolerance": 0,
323
- "N": 0,
324
- "score": 0,
325
- "reference": "https://iopscience.iop.org/article/10.1088/0034-4885/75/8/086901",
326
- "reason": ""
327
- },
328
- {
329
- "category": "theory",
330
- "question": "The Wouthuysen–Field effect is important during the dark ages before the formation of the first stars.",
331
- "choices": {
332
- "A": "yes",
333
- "B": "no",
334
- "C": "dunno"
335
- },
336
- "answer": {
337
- "type": "string",
338
- "enum": [
339
- "A",
340
- "B",
341
- "C"
342
- ],
343
- "description": "Your selected answer (A, B, or C)"
344
- },
345
- "ideal": "B",
346
- "task": 5,
347
- "tolerance": 0,
348
- "N": 0,
349
- "score": 0,
350
- "reference": "https://iopscience.iop.org/article/10.1088/0034-4885/75/8/086901",
351
- "reason": "The Wouthuysen–Field effect is present when there are lyman-alpha photons available, which is after the first stars form."
352
- },
353
- {
354
- "category": "theory",
355
- "question": "The 21-cm photons are created from the radiative cascade of an electron from the n=2 level back to one of the hyperfine levels of the n=1 ground state.",
356
- "choices": {
357
- "A": "yes",
358
- "B": "no",
359
- "C": "dunno"
360
- },
361
- "answer": {
362
- "type": "string",
363
- "enum": [
364
- "A",
365
- "B",
366
- "C"
367
- ],
368
- "description": "Your selected answer (A, B, or C)"
369
- },
370
- "ideal": "B",
371
- "task": 5,
372
- "tolerance": 0,
373
- "N": 0,
374
- "score": 0,
375
- "reference": "https://iopscience.iop.org/article/10.1088/0034-4885/75/8/086901",
376
- "reason": "This statement describes the Wouthuysen–Field effect not how 21-cm photons are created."
377
- },
378
- {
379
- "category": "theory",
380
- "question": "When the magnetic field is perpendicular to the line of sight, the electron undergoes circular motion about the magnetic field lines, causing its acceleration vector to rotate with time, resulting in circularly polarised radiation to the observer.",
381
- "choices": {
382
- "A": "yes",
383
- "B": "no",
384
- "C": "dunno"
385
- },
386
- "answer": {
387
- "type": "string",
388
- "enum": [
389
- "A",
390
- "B",
391
- "C"
392
- ],
393
- "description": "Your selected answer (A, B, or C)"
394
- },
395
- "ideal": "B",
396
- "task": 5,
397
- "tolerance": 0,
398
- "N": 0,
399
- "score": 0,
400
- "reference": "",
401
- "reason": "This happens when they are parallel."
402
- },
403
- {
404
- "category": "theory",
405
- "question": "What is the angle between the magnetic field and the line of sight that would result in purely circularly polarised radiation?",
406
- "choices": {
407
- "A": "0 degrees",
408
- "B": "45 degrees",
409
- "C": "90 degrees",
410
- "D": "it has nothing to do with the angle"
411
- },
412
- "answer": {
413
- "type": "string",
414
- "enum": [
415
- "A",
416
- "B",
417
- "C",
418
- "D"
419
- ],
420
- "description": "Your selected answer (A, B, or C)"
421
- },
422
- "ideal": "A",
423
- "task": 5,
424
- "tolerance": 0,
425
- "N": 0,
426
- "score": 0,
427
- "reference": "",
428
- "reason": ""
429
- },
430
- {
431
- "category": "theory",
432
- "question": "Which radiation is the foreground dominated by in the frequency range relevant to 21-cm cosmology?",
433
- "choices": {
434
- "A": "cosmic microwave background",
435
- "B": "synchrotron radiation",
436
- "C": "dust free-free emission"
437
- },
438
- "answer": {
439
- "type": "string",
440
- "enum": [
441
- "A",
442
- "B",
443
- "C"
444
- ],
445
- "description": "Your selected answer (A, B, or C)"
446
- },
447
- "ideal": "B",
448
- "task": 5,
449
- "tolerance": 0,
450
- "N": 0,
451
- "score": 0,
452
- "reference": "https://iopscience.iop.org/article/10.1088/0034-4885/75/8/086901",
453
- "reason": ""
454
- },
455
- {
456
- "category": "experiment",
457
- "question": "What is the statistical approach adopted in the REACH global 21-cm experiment?",
458
- "choices": {
459
- "A": "Bayesian inference",
460
- "B": "frequentist statistics",
461
- "C": "neither"
462
- },
463
- "answer": {
464
- "type": "string",
465
- "enum": [
466
- "A",
467
- "B",
468
- "C"
469
- ],
470
- "description": "Your selected answer (A, B, or C)"
471
- },
472
- "ideal": "A",
473
- "task": 5,
474
- "tolerance": 0,
475
- "N": 0,
476
- "score": 0,
477
- "reference": "https://academic.oup.com/mnras/article/506/2/2041/6307526",
478
- "reason": ""
479
- },
480
- {
481
- "category": "experiment",
482
- "question": "In a Bayesian framework, which quantity is used to compare different models?",
483
- "choices": {
484
- "A": "likelihood",
485
- "B": "Bayesian evidence",
486
- "C": "posterior probability distribution"
487
- },
488
- "answer": {
489
- "type": "string",
490
- "enum": [
491
- "A",
492
- "B",
493
- "C"
494
- ],
495
- "description": "Your selected answer (A, B, or C)"
496
- },
497
- "ideal": "B",
498
- "task": 5,
499
- "tolerance": 0,
500
- "N": 0,
501
- "score": 0,
502
- "reference": "https://academic.oup.com/mnras/article/506/2/2041/6307526",
503
- "reason": ""
504
- },
505
- {
506
- "category": "theory",
507
- "question": "What is the spin temperature of neutral hydrogen defined by the kinetic temperature of hydrogen atomsin the context of 21-cm cosmology?",
508
- "choices": {
509
- "A": "the temperature characterising the relative population of the hyperfine states",
510
- "B": "the kinetic temperature of hydrogen atoms",
511
- "C": "the temperature of the cosmic microwave background"
512
- },
513
- "answer": {
514
- "type": "string",
515
- "enum": [
516
- "A",
517
- "B",
518
- "C"
519
- ],
520
- "description": "Your selected answer (A, B, or C)"
521
- },
522
- "ideal": "A",
523
- "task": 5,
524
- "tolerance": 0,
525
- "N": 0,
526
- "score": 0,
527
- "reference": "https://iopscience.iop.org/article/10.1088/0034-4885/75/8/086901",
528
- "reason": ""
529
- },
530
- {
531
- "category": "theory",
532
- "question": "Which of the following statements provides the most precise description of the Wouthuysen-Field mechanism",
533
- "choices": {
534
- "A": "The absorption of Lyman-alpha photons heats the hydrogen gas directly, coupling its kinetic temperature to the spin temperature.",
535
- "B": "Lyman-alpha photons yield a thermal equilibrium between the 21-cm spin temperature and the temperature of the Lyman-alpha radiation field.",
536
- "C": "The repeated scattering of Lyman-alpha photons repopulate the hydrogen hyperfine levels, driving the 21-cm spin temperature to the kinetic temperature of the gas."
537
- },
538
- "answer": {
539
- "type": "string",
540
- "enum": [
541
- "A",
542
- "B",
543
- "C"
544
- ],
545
- "description": "Your selected answer (A, B, or C)"
546
- },
547
- "ideal": "C",
548
- "task": 5,
549
- "tolerance": 0,
550
- "N": 0,
551
- "score": 0,
552
- "reference": "https://iopscience.iop.org/article/10.1088/0034-4885/75/8/086901",
553
- "reason": ""
554
- },
555
- {
556
- "category": "theory",
557
- "question": "When does Lyman-alpha coupling become effective?",
558
- "choices": {
559
- "A": "when Wouthuysen-Field coupling rate exceeds the Hubble expansion rate",
560
- "B": "when the first stars form and emit Lyman-alpha radiation",
561
- "C": "when the universe becomes dominated by dark energy"
562
- },
563
- "answer": {
564
- "type": "string",
565
- "enum": [
566
- "A",
567
- "B",
568
- "C"
569
- ],
570
- "description": "Your selected answer (A, B, or C)"
571
- },
572
- "ideal": "A",
573
- "task": 5,
574
- "tolerance": 0,
575
- "N": 0,
576
- "score": 0,
577
- "reference": "https://academic.oup.com/mnras/article/367/1/259/1018616",
578
- "reason": ""
579
- },
580
- {
581
- "category": "theory",
582
- "question": "Why is the 21-cm line unobservable during the dark ages even though neutral hydrogen is abundant",
583
- "choices": {
584
- "A": "the spin temperature is coupled to the CMB temperature",
585
- "B": "the optical depth is too high",
586
- "C": "hydrogen is too cold to emit radiation"
587
- },
588
- "answer": {
589
- "type": "string",
590
- "enum": [
591
- "A",
592
- "B",
593
- "C"
594
- ],
595
- "description": "Your selected answer (A, B, or C)"
596
- },
597
- "ideal": "A",
598
- "task": 5,
599
- "tolerance": 0,
600
- "N": 0,
601
- "score": 0,
602
- "reference": "",
603
- "reason": ""
604
- },
605
- {
606
- "category": "theory",
607
- "question": "Cross-correlating 21-cm experiments with galaxy surveys does not provide significant constraints on which of the following?",
608
- "choices": {
609
- "A": "the total matter density of the universe,",
610
- "B": "the escape fraction of ionising photons from the observed galaxies",
611
- "C": "the astrophysical bias of the observed galaxy population",
612
- "D": "it constrains all of the above"
613
- },
614
- "answer": {
615
- "type": "string",
616
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617
- "A",
618
- "B",
619
- "C",
620
- "D"
621
- ],
622
- "description": "Your selected answer (A, B, C, or D)"
623
- },
624
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625
- "task": 5,
626
- "tolerance": 0,
627
- "N": 0,
628
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629
- "reference": "",
630
- "reason": ""
631
- },
632
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633
- "category": "theory",
634
- "question": "What is the statistical weight ratio of the hydrogen hyperfine levels at n=1?",
635
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636
- "A": "1",
637
- "B": "2",
638
- "C": "3",
639
- "D": "4"
640
- },
641
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642
- "type": "string",
643
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644
- "A",
645
- "B",
646
- "C",
647
- "D"
648
- ],
649
- "description": "Your selected answer (A, B, C, or D)"
650
- },
651
- "ideal": "C",
652
- "task": 5,
653
- "tolerance": 0,
654
- "N": 0,
655
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656
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657
- "reason": ""
658
- },
659
- {
660
- "category": "theory",
661
- "question": "21-cm forest refers to the appearance of lines from regions of neutral gas at different distances to the CMB.",
662
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663
- "A": "yes",
664
- "B": "no",
665
- "C": "dunno"
666
- },
667
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668
- "type": "string",
669
- "enum": [
670
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671
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672
- "C"
673
- ],
674
- "description": "Your selected answer (A, B, or C)"
675
- },
676
- "ideal": "B",
677
- "task": 5,
678
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679
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680
- "score": 0,
681
- "reference": "https://iopscience.iop.org/article/10.1088/0034-4885/75/8/086901",
682
- "reason": "It is with respect to the radio source, not the CMB."
683
- },
684
- {
685
- "category": "theory",
686
- "question": "The amplitude of the EDGES global 21-cm profile can be explained by warm dark matter.",
687
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688
- "A": "yes",
689
- "B": "no",
690
- "C": "dunno"
691
- },
692
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693
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694
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695
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696
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697
- "C"
698
- ],
699
- "description": "Your selected answer (A, B, or C)"
700
- },
701
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702
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703
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704
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705
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706
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707
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708
- },
709
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710
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711
- "question": "In the warm dark matter scenario, the onset of star formation happens earlier than in the cold dark matter.",
712
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713
- "A": "yes",
714
- "B": "no",
715
- "C": "dunno"
716
- },
717
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718
- "type": "string",
719
- "enum": [
720
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721
- "B",
722
- "C"
723
- ],
724
- "description": "Your selected answer (A, B, or C)"
725
- },
726
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727
- "task": 5,
728
- "tolerance": 0,
729
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730
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731
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732
- "reason": ""
733
- },
734
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735
- "category": "theory",
736
- "question": "In the warm dark matter scenario, the Wouthuysen-Field coupling saturates earlier than in the lambda-CDM scenario.",
737
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738
- "A": "yes",
739
- "B": "no",
740
- "C": "dunno"
741
- },
742
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743
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744
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745
- "A",
746
- "B",
747
- "C"
748
- ],
749
- "description": "Your selected answer (A, B, or C)"
750
- },
751
- "ideal": "B",
752
- "task": 5,
753
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754
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755
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756
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757
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758
- },
759
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760
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761
- "question": "Double reionisation is likely.",
762
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763
- "A": "yes",
764
- "B": "no",
765
- "C": "dunno"
766
- },
767
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768
- "type": "string",
769
- "enum": [
770
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771
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772
- "C"
773
- ],
774
- "description": "Your selected answer (A, B, or C)"
775
- },
776
- "ideal": "B",
777
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778
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779
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780
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781
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782
- "reason": ""
783
- },
784
- {
785
- "category": "theory",
786
- "question": "Cosmic ray heating creates 21-cm signatures on larger spacial scales compared to X-ray heating.",
787
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788
- "A": "yes",
789
- "B": "no",
790
- "C": "dunno"
791
- },
792
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793
- "type": "string",
794
- "enum": [
795
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796
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797
- "C"
798
- ],
799
- "description": "Your selected answer (A, B, or C)"
800
- },
801
- "ideal": "B",
802
- "task": 5,
803
- "tolerance": 0,
804
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805
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806
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807
- "reason": "Cosmic ray heating of the IGM is short-ranged"
808
- },
809
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810
- "category": "experiment",
811
- "question": "The shape of the EDGES global 21-cm absorption profile cannot be recreated in models even with several heating contributions.",
812
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813
- "A": "yes",
814
- "B": "no",
815
- "C": "dunno"
816
- },
817
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818
- "type": "string",
819
- "enum": [
820
- "A",
821
- "B",
822
- "C"
823
- ],
824
- "description": "Your selected answer (A, B, or C)"
825
- },
826
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827
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828
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829
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830
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831
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832
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833
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834
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835
- "category": "experiment",
836
- "question": "What does foreground wedge in the delay space refer to?",
837
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838
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839
- "B": "an interferometric instrumental artifact",
840
- "C": "a region contaminated by the foregrounds"
841
- },
842
- "answer": {
843
- "type": "string",
844
- "enum": [
845
- "A",
846
- "B",
847
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848
- ],
849
- "description": "Your selected answer (A, B, or C)"
850
- },
851
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852
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853
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854
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855
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856
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857
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858
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859
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860
- "category": "experiment",
861
- "question": "Which methodologies of calibration do global 21-cm experiments use?",
862
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863
- "A": "direction dependent",
864
- "B": "direction independent",
865
- "C": "both"
866
- },
867
- "answer": {
868
- "type": "string",
869
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870
- "A",
871
- "B",
872
- "C"
873
- ],
874
- "description": "Your selected answer (A, B, or C)"
875
- },
876
- "ideal": "B",
877
- "task": 5,
878
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879
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880
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881
- "reference": "",
882
- "reason": ""
883
- },
884
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885
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886
- "question": "For 21-cm signal observations after reionisation, aiming for spatial fluctuations at the scale of ionised bubbles is appropriate.",
887
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888
- "A": "yes",
889
- "B": "no",
890
- "C": "dunno"
891
- },
892
- "answer": {
893
- "type": "string",
894
- "enum": [
895
- "A",
896
- "B",
897
- "C"
898
- ],
899
- "description": "Your selected answer (A, B, or C)"
900
- },
901
- "ideal": "B",
902
- "task": 5,
903
- "tolerance": 0,
904
- "N": 0,
905
- "score": 0,
906
- "reference": "https://iopscience.iop.org/article/10.1088/1538-3873/ab5bfd",
907
- "reason": ""
908
- },
909
- {
910
- "category": "instrumentation",
911
- "question": "How many calibrators are there in the global 21-cm experiment REACH?",
912
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913
- "A": "4",
914
- "B": "8",
915
- "C": "12"
916
- },
917
- "answer": {
918
- "type": "string",
919
- "enum": [
920
- "A",
921
- "B",
922
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923
- ],
924
- "description": "Your selected answer (A, B, or C)"
925
- },
926
- "ideal": "C",
927
- "task": 5,
928
- "tolerance": 0,
929
- "N": 0,
930
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931
- "reference": "https://link.springer.com/article/10.1007/s10686-024-09975-3",
932
- "reason": ""
933
- },
934
- {
935
- "category": "instrumentation",
936
- "question": "SKA-low antenna response is sufficiently smooth to recover the EoR signal through statistical methods.",
937
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938
- "A": "yes",
939
- "B": "no",
940
- "C": "dunno"
941
- },
942
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943
- "type": "string",
944
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945
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946
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947
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948
- ],
949
- "description": "Your selected answer (A, B, or C)"
950
- },
951
- "ideal": "B",
952
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953
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954
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955
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956
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957
- "reason": "Mutual coupling between antennas within a station makes this untrue."
958
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959
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960
- "category": "instrumentation",
961
- "question": "SKA-low antenna mutual coupling can be resolved by randomising the position and direction of the antennae.",
962
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963
-
964
- "A": "yes",
965
- "B": "no",
966
- "C": "dunno"
967
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968
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969
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970
- "enum": [
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972
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973
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974
- ],
975
- "description": "Your selected answer (A, B, or C)"
976
- },
977
- "ideal": "B",
978
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979
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980
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983
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984
- },
985
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986
- "category": "theory",
987
- "question": "Timing of Lyman-alpha coupling is well constrained by observations of high-redshift quasars, galaxies, and the CMB.",
988
- "choices": {
989
-
990
- "A": "yes",
991
- "B": "no",
992
- "C": "dunno"
993
- },
994
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995
- "type": "string",
996
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997
- "A",
998
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999
- "C"
1000
- ],
1001
- "description": "Your selected answer (A, B, or C)"
1002
- },
1003
- "ideal": "B",
1004
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1005
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1006
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1007
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1008
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1009
- "reason": ""
1010
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1011
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1012
- "category": "theory",
1013
- "question": "In the context of 21-cm cosmology, Lyman-alpha photons would travel further on a larger scale when multiple scattering is included.",
1014
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1015
-
1016
- "A": "yes",
1017
- "B": "no",
1018
- "C": "dunno"
1019
- },
1020
- "answer": {
1021
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1022
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1023
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1024
- "B",
1025
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1026
- ],
1027
- "description": "Your selected answer (A, B, or C)"
1028
- },
1029
- "ideal": "B",
1030
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1031
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1032
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1034
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1035
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1036
- },
1037
- {
1038
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1039
- "question": "In most scenarios (except in cases like with weak X-ray heating), multiple scattering plays an important role at lower redshift where Lyman-alpha coupling saturates and the 21-cm fluctuations are dominated by heating processes.",
1040
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1041
-
1042
- "A": "yes",
1043
- "B": "no",
1044
- "C": "dunno"
1045
- },
1046
- "answer": {
1047
- "type": "string",
1048
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1050
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1051
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1052
- ],
1053
- "description": "Your selected answer (A, B, or C)"
1054
- },
1055
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1056
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1058
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1059
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1060
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1061
- "reason": "At higher redshift."
1062
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1063
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1064
- "category": "theory",
1065
- "question": "Lower X-ray efficiency would make reionisation more homogeneous.",
1066
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1067
-
1068
- "A": "yes",
1069
- "B": "no",
1070
- "C": "dunno"
1071
- },
1072
- "answer": {
1073
- "type": "string",
1074
- "enum": [
1075
- "A",
1076
- "B",
1077
- "C"
1078
- ],
1079
- "description": "Your selected answer (A, B, or C)"
1080
- },
1081
- "ideal": "B",
1082
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1083
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1084
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1086
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1087
- "reason": "Higher X-ray efficiency."
1088
- },
1089
- {
1090
- "category": "instrumentation",
1091
- "question": "In 21-cm experiments, impedance mismatch between the low noise amplifiers and optical transmitters causes power from the foreground signals to appear at lower delays, potentially contaminating the EoR window.",
1092
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1093
-
1094
- "A": "yes",
1095
- "B": "no",
1096
- "C": "dunno"
1097
- },
1098
- "answer": {
1099
- "type": "string",
1100
- "enum": [
1101
- "A",
1102
- "B",
1103
- "C"
1104
- ],
1105
- "description": "Your selected answer (A, B, or C)"
1106
- },
1107
- "ideal": "B",
1108
- "task": 5,
1109
- "tolerance": 0,
1110
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1111
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1112
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1113
- "reason": "it would appear at higher delays, not lower delays."
1114
- },
1115
- {
1116
- "category": "experimentation",
1117
- "question": "In a delay power spectrum for 21-cm experiments, which k-modes should exhibit the lowest foreground-to-signal ratio?",
1118
- "choices": {
1119
-
1120
- "A": "those above the horizon limit",
1121
- "B": "those below the horizon limit",
1122
- "C": "there is no difference"
1123
- },
1124
- "answer": {
1125
- "type": "string",
1126
- "enum": [
1127
- "A",
1128
- "B",
1129
- "C"
1130
- ],
1131
- "description": "Your selected answer (A, B, or C)"
1132
- },
1133
- "ideal": "A",
1134
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1135
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1136
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1138
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1139
- "reason": ""
1140
- },
1141
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1142
- "category": "instrumentation",
1143
- "question": "What data types are correlation saved to in measurement set in radio astronomy?",
1144
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1145
-
1146
- "A": "COMPLEX*8",
1147
- "B": "COMPLEX*16",
1148
- "C": "COMPLEX*32"
1149
- },
1150
- "answer": {
1151
- "type": "string",
1152
- "enum": [
1153
- "A",
1154
- "B",
1155
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1156
- ],
1157
- "description": "Your selected answer (A, B, or C)"
1158
- },
1159
- "ideal": "A",
1160
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1161
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1162
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1163
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1164
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1165
- "reason": ""
1166
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1167
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1168
- "category": "theory",
1169
- "question": "Other parameters being the same, decreasing density of matter will increase the width of the 21-cm absorption signal.",
1170
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1171
-
1172
- "A": "yes",
1173
- "B": "no",
1174
- "C": "dunno"
1175
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1176
- "answer": {
1177
- "type": "string",
1178
- "enum": [
1179
- "A",
1180
- "B",
1181
- "C"
1182
- ],
1183
- "description": "Your selected answer (A, B, or C)"
1184
- },
1185
- "ideal": "B",
1186
- "task": 5,
1187
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1188
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1189
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1190
- "reference": "https://articles.adsabs.harvard.edu/pdf/1977SvAL....3..155V",
1191
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1192
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1193
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