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[IPTA-cs] (1) Metastable strings (2) Subgroups
- Subject: [IPTA-cs] (1) Metastable strings (2) Subgroups
- From: Kai Schmitz <kai schmitz cern ch>
- Date: Fri, 28 Jan 2022 14:03:40 +0100
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Hi All,
A few comments on two topics: (1)
Metastable cosmic strings and (2) Forming smaller subgroups. @Paul,
@Nihan, please have a look at my question below.
(1) Metastable cosmic strings:
A few of you were reaching out to me
after yesterday's call because they are interested in my
"metastable cosmic string" proposal. This is great! I indeed think
that "metastable strings" are an option that we should explore,
because they are (a) well motivated from the particle physics
perspective and (b) promise to significantly improve the quality
of our fit---if strings happen to decay in the right time window
in the early Universe. More precisely, as you can see in our paper
https://arxiv.org/abs/2107.04578, the U(1) and GUT symmetry
breaking scales that respectively determine the cosmic-string
tension and the GUT monopole mass need to be separated by a factor
8 or 9 or so, see the left panel of Fig. 3. This is a somewhat
specific value, but there is certainly no strong fine-tuning
involved, and values of this order of magnitude are definitely
plausible and realistic in concrete GUT models. See, e.g., Eq.
(23) in
https://arxiv.org/abs/2102.08923, which actually
"predicts" a value of 8 in a simple SU(2) x U(1) model.
(2) Subgroups:
We have now reached a good point where
we can start thinking about forming smaller subgroups. How about
the following three groups as a first proposal:
- Subgroup 1: Implementation into
ENTERPRISE (first task: implementation of the look-up table I
generated shortly before Christmas)
- Subgroup 2: Metastable cosmic strings
(first task: derive a closed analytical _expression_ for the GW
spectrum)
- Subgroup 3: Your suggestion (e.g.,
superstrings, first task in this case: think about going beyond
the simple 1/p rescaling, see, e.g.,
https://arxiv.org/abs/1606.05585)
If I understand correctly, Paul and
Nihan would be interested in contributing to subgroup 1, even
though they might need some time, because of a few other things
keeping them busy at the moment. In addition, it would be great if
we could attract more PTA members with ENTERPRISE experience that
could help us with the implementation. @Paul, @Nihan,
do you think it would make sense to send around a mail on a big
IPTA mailing list or something like that, in order to solicit more
team members with ENTERPRISE experience?
Another comment is that I will take up
a tenure-track assistant professor position at the University of
Münster in May. Initially, I will have (at least) two PhD students
in my group, and I will definitely suggest to one of them to
become a member of our team. If the student should be interested,
I would propose to them to spend some time with ENTERPRISE, so
that they could help us with the implementation of the signals
that we are interested in.
As for the second subgroup, I would
suggest that we should have a meeting in two weeks with
everyone who's interested in doing some actual analytical
pen-on-paper calculations on metastable cosmic strings. If you are
interested, please indicate your preferred time slot in the
following doodle:
Finally, regarding the third subgroup:
Please feel free to make suggestions. Cosmic superstrings sound
like an interesting possibility to me, especially because they may
also allow us to improve the quality of the fit. But most of all,
I would like to hear your suggestions.
Talk to you soon and have a great
weekend, everyone!
Best regards, Kai.
On 1/27/22 18:21, Kai Schmitz via
IPTA-cosmic-strings wrote:
Hi All,
Thanks a lot for the great meeting today. Here are the slides
and the recording:
Slides:
https://docs.google.com/presentation/d/1t-4FTycO2hWpfv1KzBAkSrgcYif6HWKnKBxkS756Smk/edit?usp=sharing
Recording:
https://drive.google.com/file/d/181IPQWW0EIVPHAp2rlX7InPhX9onamgl/view?usp=sharing
The tentative date for the next meeting is Thursday,
February 24, 2022 at 15:00 UTC. However, if there should
new results from a first Enterprise run at an earlier point, we
can as well spontaneously schedule an earlier meeting. In the
meantime, let's continue the discussion here on the mailing
list.
Speaking of that, let me provide you with a few more details on
our analysis of metastable cosmic strings in
[1] https://arxiv.org/abs/2107.04578
which builds upon earlier work by Louis Leblond, Benjamin
Shlaer, and Xavier Siemens:
[2] https://arxiv.org/abs/0903.4686
This earlier paper focuses exclusively on gravitational waves
from string segments with monopoles on both ends, estimating the
GW spectrum based on and extending the following calculation by
Xavier Martin and Alexander Vilenkin
[3] https://arxiv.org/abs/gr-qc/9612008
What we now do in our paper from last year is to extend the
analysis from segments-only to the full scenario including both
types of animals, closed loops and segments. We distinguish in
particular between three populations: (a) closed loops that are
chopped off from long strings, (b) segments originating from
monopole nucleation on long strings, and (c) segments
originating from monopole nucleation on closed loops. For closed
loops, we assume that GW emission is dominated by cusps (q =
4/3), while for segments we use the Martin-Vilenkin result (q=1,
up to some cutoff mode number). Moreover, in order to estimate
the number densities of all three populations, we work with
transport equations [see Eq. (A.1) in https://arxiv.org/abs/2107.04578],
similar to those employed by Leblond, Shlaer, and Siemens. We
solve these equations in some cases analytically, in other cases
numerically, and make sure that we reproduce the known results
for stable strings at early times (i.e., the results of your
numerical simulations). The transport equations allow us in
particular to describe how one population (e.g., closed strings)
can act as the source of another population (e.g., segments
originating from monopole nucleation on closed loops).
And again, I invite you to have a closer look at our paper. My
impression is that metastable strings could give us a
considerably better fit to the data than stable cosmic strings.
Plus, they would be well motivated from the perspective of grand
unification. (Of course the lifetime would need to fall into a
somewhat narrow window, as J.J. was pointing out.)
In a more general sense, my question is whether we should
really restrict ourselves to only one benchmark scenario that
can parametrized by, say, just one free parameter (log Gmu)? Or
whether we want to consider slightly more general scenarios,
which may be motivated by different physics arguments (as Ken
was emphasizing). We could definitely have a look into cosmic
superstrings and see whether they improve the quality of the
fit. And we could study Nambu-Goto strings in dependence of two
parameters: (a) their tension and (b) their lifetime. In this
case, we could present our results in a 2D parameter plot
(tension versus lifetime), which would trivially also cover the
case of stable cosmic strings (namely, in the parameter region
where the lifetime becomes longer and longer). Let me know what
you think.
And finally, let me / us know if you have got further
questions, ideas, comments? Which other directions would you
like to explore? Where and how would you like to contribute to
the project? Anything we should change about the style of our
meetings? Should we stick to the current format or try something
else? Any input or suggestions are welcome.
Thanks again and talk to you soon!
Best regards, Kai.