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07:04
Hello world
08:00
Hi
Now I am available.
but its possible that I have to leave now and then!
08:18
okay I was rethinking about the quaternioninc representations
they still are the sum of two complex conjugate irreducible representations
except that this time the complex irrep is isomorphic to its complex conjugate
I remember a little
so we still have decomposition of real representations into real irreps
but some of them are a bit less rigid than what we have in the complex case
and anyway it shouldn't interfere with what we do
08:38
left and back.
I quickly paste the Referees point:
btw. have you got access to the complete referee statements?
I'm not sure
I have a version from june 12 with some referee comment
here the one statement6) The Authors wrote on page 3 of the text that they use only the real representations instead of complex. It can be understood as a ban on the use of Schur's lemmas for some axial groups.
(The right constructions were used in SM). This peculiar point is important in the analysis of the transformations for gradients, which still has to be done correctly for point groups with complex one-dimensional representations (the note at the top of page S2 is incorrect in this case and should not be used).
"the note at the top of page S2" is that something in our paper ?
also what is SM ?
do you want me to send you the comlpete statements or would you prefer that "I walk us thorough"?
Supplementary Material
S2 is the second page of that.
that page is about Schur functors
oh wait
"Finally, if Γ is a real irreducible representation by a group G, then
Sym 2 (Γ) always has exactly one totally symmetric Γ 0 component in its decomposition, so that
for any two dimensional real irreducible representation E"
that is wrong
but
wait no it is right
08:45
:-)
Sym²
it is Alt² that gets all the extra Gamma0s
in case of a sum of conjugate pairs
So you have the current version?
But wait I'll send you the real current submission version by email
I don't think my version has the same referer comments
the note on S2 is true but I might have to explain it a bit more then
I sent it, please go through that I'll be away for 20 min
I think that's the one I have
I still can't find the comments you are quoting
09:13
the classical result is that an occurence of the trivial rep in Sym²(rho) corresponds to a G-linear automorphism V -> V, and then by Schur's lemma, there is only one of them
but that's over C
over R, in case rho = r + r'
actually they might be right
I have to check
Sym²(rho) = Sym²(r) + Sym²(r') + r * r'
:(
I was so sure they would be split ?
I do remember checking this
let's check on the cyclic group of order 3
ahaha
I think there is a dual thing I forgot
but then the Schur's lemma argument doesn't work as is
it's not Sym²(r) that corresponds to an automorphism
it's r' * r
Sym²(r) is more about symmetric bilinear forms
probably
so in Sym²(r+r') the Gamma0 component comes from r * r'
alright, the dual representation
is given by rho*(g) = transpose of rho(inverse of g)
and so an automorphism of V
corresponds to a Gamma0 component in the tensor product of V and V*
... that still doesn't give the "easy" proof that there is exactly one Gamma0 component in rho tensor rho when rho is a complex irreducible representation
well it does for unitary representations
and every finite group representation is unitarizable if I'm reading wikipedia correctly
09:43
@mercio Sure these are the referee comments. I will send them to you as well. But mind that then you still miss the comments from the first round of reviewing. We might ome to that later in case of need. I anyway suggest we two now and here focus on the specific numbered issie list from rev 4 for now.
The problem is that the whole thing is already very confusing with two rounds of reviewing ...
So lets try to stay focused.
@mercio Hm why can't we just go back to reps over C for the proof, and check that we have all groups included that matter?
there are also some elementary proofs that if A is a matrix of finite order then tr(inverse of A) = conjugate of tr(A) so I guess that works
I think they are talking about the (S1) statement
where I say that Sym²(rho) has exactly one Gamma0 component when rho is a real irreducible representation
I think the usual argument, over C, goes like this
btw. does comment 7 help here?
I still have not found comment 6
which page are they on ?
09:51
I have submitted another email
with the two complete referee statements
I got it
7) Many constructions would be much shorter and clearer if a known (and easily inferred)
expression were used: the symmetrized square of the representation Г ( dimГ = n ) has
dimension n(n+1)/2, and n(n-1)/2 corresponds to the antisymmetrized square
yes but the dimension doesn't tell everything there is to know about a representation ?
Some statements are well known from the theory of vibrations. For
example, the matrices of the (x,y,z) coordinates representation and the corresponding
infinitesimal rotations ( i.e., the projections of the momentum) differ only in the factor – the
determinant of the matrix – and therefore are simultaneously reducible or irreducible.
well I don't know anything about what is well known or not in physics
and I don't know what they mean with "differ only in the factor"
(the note at the top of page S2 is incorrect in this case and
should not be used).
the note is correct but is phrased in a way that might look wrong
I should think about improving that part
also those tables need some vertical bars
10:16
here is a problem. at this stage we need to carefully protocol and comment all changes
do you know git?
I haven't used it much
me not either I just start learning it. But I think it would be the right tool now.
possibly
Well on the other hand if we only do punctual changes one after the other we can do without it as well .
For git in any case we'd need to set up a server. I had the remote hope you would be an experienced git user. But in this case maybe its easier without
I am wondering what background that referee has. I am certain he is no chemist
Y and Yh for what we call I and Ih is very uncommon.
don't worry, I and Ih is very uncommon too
10:26
:-)
from where I come from
... does he want us to include definitions of vector spaces and representations and tensor products ?
no idea. I have already complaint about the very unspecific comments, its a really tough one, that paper ...
Well we both should try to fix 6. now
I have to admit I chuckled inside when he asked for a "definition statement proof" since I sometimes feel that physicists do the opposite in their writings
"experimental result - computations - therefore we should use this definition because it works"
10:29
there are so many aspects, this work is the worst in trouble making I ever had
I'm sorry it sounds hard
not at all your faut
fault
I see people wanting math stuff to be moved all to the supplementary section
then the next one wanting the opposite
exaclty
one wants it to be shortend to 2 pages
the other one extended to 3 publications ...
that all depends on soft criteria
the fact that it relies on some math stuff does sound like it makes the procedure a bit wonky
we are all accustommed to our own things and ways of describing things
10:31
yes
and in a sense its heavily interdisciplinary
Its very hard to focus on certain readership
I tried to and the the referess imply different readerships
but mostly ones that are different from themselves as well
its a terrible mess, to be honest :(
But then I think its mostly questions of style
I am aware that it is not greatly presented as it is, but I don't know how to do it substantially better.
In no case on two pages like ref 3 wanted
rev 4 has a very good understadning of the physics and maths but none for the field on which it should have the largest impact
ah yes there was this other referee
rev3 got some things quite wrong to begin with and that caused also lots of misunderstanding
apparently we said that D2d was abelian ?
Yeah I am so sorry
that was huge stupidity
I don't even remember what D2d is
10:38
He suggested to call then abelian and non-abelian
which is wrong (as we know)
so I wanted to give a counter example
and then I got it wrong which caused troubles in this thrid round
I do remember one of the D2x ones being tricky
but they both understand now that its not non-abelian
and not being in the same family as his D3x D4x ... friends
10:39
well all the S2n are ones
all with pairs of imaginary 1D irreps
its actually the 1D imaginary that make the troubles
yes.
I'm going to read his group theory book
a little
but now he understood it and suggests stil not to use Kaaa, Kae and Kt but G1, G2, G3,
and call them 2-D represented which i think is again less precise and G_1 for me is one certain group
instead a family of groups ....
well I think G1 G2 G3 would be fine
the referee is less of a problem and has less clear insight.
@mercio Well, than kwhy not
one just has to define them properly
"1D, 2D and 3D represented" as he suggests is simply not good enough I think
anyway we should try to fix the most severe thing and that is 6. of rev4
because there are 2D irreps in G3 as well
yeah but they're not faithful
10:47
and there are 5D irreps in G3
and yeah I don't want to suggest there are families G4 G5 G6...
anyway
So the full formulated defintion is G1= 1D over R, G2= 2D but no higher over R, and G3= the rest.
I don't see a way to make it simpler
yeah that would clash if somebody would read G3 = 3D but no higher
Its simply not a trivial partition.
the way I have them in my head is G1 = faithful 3d reps are all of the form a+a+a ; G2 = faithful 3d reps are all of the form a+e ; G3 = faithful 3d reps are all of the form t
and then it's a nontrivial result that there is no group having two kinds of faithful 3d rep
10:51
yes.
anyway, the usual equivalent of the note (S1) is that for a complex rep rho, there is exactly one Gamma0 in rho tensor conjugate(rho)
The most "cryspy" way is to call the 3 or higher represented ones a name. And say all non-NAME that are not 1D over R.
ok
because conjugate(rho) = dual of rho, then rho tensor dual of rho = maps from V to V, and invariant maps = G-automorphism, and Schur's lemma says there is only one
and I am saying that for a real irrep rho there is exactly one Gamma0 is Sym²(rho)
but in fact
depending on the kind of irrep rho is there can be 1,2, or 4 Gamma0s in rho²
which is I think what he is thinking about
because rho² would be the real equivalent of rho * conjugate of rho
but not in the point groups afaik?
some of the point groups have 2 in rho²
it's always exactly one in the symmetric part
10:55
oh yes!
and 0,1, or 3 in the alternate part
and that's something I haven't expanded upon
is there an example of 3?
yes with quaternionic representations
the archetypal example being the quaternion group
10:56
ok but not in the point groups
I don't think so
but I would have to check
in G3
I am relatively sure, but checking is better
There is only very few e
I don't think e can be quaternionic
it can only happen on dimension at least 4
the quaternion group doesn't have a faithful representation in R³
I dont think so. It doesnt ring a bell ...
if its not T it cant be anything I guess
but T is A4
if i rem correctly ?
link me your friend's website again ?
11:00
Oh and there is S4
did you notive btw its a html programm
?
yeah
Everything is computed ...
:-)
a pitty he hates complex numbers ... :-D
if rho = r1 + r2 where r1 and r2 are different (and conjugate of each other) then rho² = r1²+r2²+2r1r2, so they are 2 Gamma0 because there are 2r1r2
if rho = 2r (with r complex and isomorphic to its conjugate) then rho² = 4r²
and that will be 4 Gamma0
but 3 of them are in the Alternate part
that's the quaternionic case
11:04
OK.
so for example for the representation of a cyclic group (n >= 3) on a plane with rotations
it has two Gamma0 in its square
and that corresponds to two automorphisms
well dimension 2 rather
while Schur's lemma would say there can only be homotheties
in this case you will also have rotations
those are also endomorphisms that are compatible with the action of G
I mean its exactly those which spoil the fun just using reps over C
I'm kinda sad there is no quaternionic point group
11:12
sorry for that
S2?
well I looked at the tables and only I and Ih had irreps of dimension > 3 and apparently they weren't quaternionic
sorry S4
sure ..
not is only the 6 of them in Kt / G3
I don't think any of the symmetric groups have quaternionic stuff but I could be very very wrong
my intuition fails me
I know we have a thing to biject their C irreps with Young tableaux
Have you heared that soemthing like Jahn-Teller exists only in prime dimension spaces?
lol
no
11:15
Yeah
So in real 4D space there would be degeneracies that cannot be lifted by vibrational motions ....
don't break spacetime now
so I don't know if I can just add a remark
saying there can be one Gamma0 in the Alternate part
or if I have to explain more and prove it
Well it would be actually also not bad to change the whole prove, that would calm down the editor a bit
:'(
11:19
But as you like
the only point is to adress problem 6.
and that the paper is correct in the end
This peculiar point is important in the analysis of the
transformations for gradients, which still has to be done correctly for point groups with complex
one-dimensional representations
the transformations for gradients ?
the calculation you do, i think
−i (r′ ×∇′) = −i (Ur×U∇) = (U ×U)l
∇′ = U ∇ because U is orthogonal,
ah, so the gradient was for the nabla
yes, that is the same (for some)
 
4 hours later…
15:39
So please feel free anytime to give a message if you have a good fix. I would like to try resubmission during the weekend if possible.

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