×
Well done. You've clicked the tower. This would actually achieve something if you had logged in first. Use the key for that. The name takes you home. This is where all the applicables sit. And you can't apply any changes to my site unless you are logged in.

Our policy is best summarized as "we don't care about _you_, we care about _them_", no emails, so no forgetting your password. You have no rights. It's like you don't even exist. If you publish material, I reserve the right to remove it, or use it myself.

Don't impersonate. Don't name someone involuntarily. You can lose everything if you cross the line, and no, I won't cancel your automatic payments first, so you'll have to do it the hard way. See how serious this sounds? That's how serious you're meant to take these.

×
Register


Required. 150 characters or fewer. Letters, digits and @/./+/-/_ only.
  • Your password can’t be too similar to your other personal information.
  • Your password must contain at least 8 characters.
  • Your password can’t be a commonly used password.
  • Your password can’t be entirely numeric.

Enter the same password as before, for verification.
Login

Grow A Dic
Define A Word
Make Space
Set Task
Mark Post
Apply Votestyle
Create Votes
(From: saved spaces)
Exclude Votes
Apply Dic
Exclude Dic

Click here to flash read.

Hawking discovery that black holes can evaporate through radiation emission
has posed a number of questions that with time became fundamental hallmarks for
a quantum theory of gravity. The most famous one is likely the information
paradox, which finds an elegant explanation in the Page argument suggesting
that a black hole and its radiation can be effectively represented by a random
state of qubits. Leveraging the same assumption, we ponder the extent to which
a black hole may display emergent symmetries, employing the entanglement
asymmetry as a modern, information-based indicator of symmetry breaking. We
find that for a random state devoid of any symmetry, a $U(1)$ symmetry emerges
and it is exact in the thermodynamic limit before the Page time. At the Page
time, the entanglement asymmetry shows a finite jump to a large value. Our
findings imply that the emitted radiation is symmetric up to the Page time and
then undergoes a sharp transition. Conversely the black hole is symmetric only
after the Page time.

Click here to read this post out
ID: 563882; Unique Viewers: 0
Unique Voters: 0
Total Votes: 0
Votes:
Latest Change: Nov. 22, 2023, 7:30 a.m. Changes:
Dictionaries:
Words:
Spaces:
Views: 9
CC:
No creative common's license
Comments: