Stringy landscape v.s higgs fine tuning

ensabah6
Messages
691
Reaction score
0
Susy has been offered as a way to stabilize the Higgs sector from radiative corrections, on the argument that w/o SUSY the higgs expansion would have to be fine-tuned to 32 decimal places.

But string theory landscape posits 10^500 different compactification schemes w/anthropic principle offered to select one. Is this an improvement? why not suggest a multiverse of higgs potentials with ours being one of many (and hence fined tuned)/
 
Physics news on Phys.org
The string landscape is only an improvement if you can show both that significantly less fine-tuned vacua are totally inhospitable to intelligent life of any kind and that all (or at least a very large sampling) of the sting vacua actually exist.

In a sense, the string landscape is exactly what you're suggesting for the Higgs potential, only extended to a larger parameter set. The only difference is that the string landscape is justified by what might be a more fundamental theory than what we already know about the universe, while an ad hoc multiverse is not.
 
Toponium is a hadron which is the bound state of a valance top quark and a valance antitop quark. Oversimplified presentations often state that top quarks don't form hadrons, because they decay to bottom quarks extremely rapidly after they are created, leaving no time to form a hadron. And, the vast majority of the time, this is true. But, the lifetime of a top quark is only an average lifetime. Sometimes it decays faster and sometimes it decays slower. In the highly improbable case that...
I'm following this paper by Kitaev on SL(2,R) representations and I'm having a problem in the normalization of the continuous eigenfunctions (eqs. (67)-(70)), which satisfy \langle f_s | f_{s'} \rangle = \int_{0}^{1} \frac{2}{(1-u)^2} f_s(u)^* f_{s'}(u) \, du. \tag{67} The singular contribution of the integral arises at the endpoint u=1 of the integral, and in the limit u \to 1, the function f_s(u) takes on the form f_s(u) \approx a_s (1-u)^{1/2 + i s} + a_s^* (1-u)^{1/2 - i s}. \tag{70}...
Back
Top