×
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.

The promise of gyrochronology is that given a star's rotation period and
mass, its age can be inferred. The reality of gyrochronology is complicated by
effects other than ordinary magnetized braking that alter stellar rotation
periods. In this work, we present an interpolation-based gyrochronology
framework that reproduces the time- and mass-dependent spin-down rates implied
by the latest open cluster data, while also matching the rate at which the
dispersion in initial stellar rotation periods decreases as stars age. We
validate our technique for stars with temperatures of 3800-6200 K and ages of
0.08-2.6 gigayears (Gyr), and use it to reexamine the empirical limits of
gyrochronology. In line with previous work, we find that the uncertainty floor
varies strongly with both stellar mass and age. For Sun-like stars (5800 K),
the statistical age uncertainties improve monotonically from $\pm$38% at 0.2
Gyr to $\pm12$% at 2 Gyr, and are caused by the empirical scatter of the
cluster rotation sequences combined with the rate of stellar spin-down. For
low-mass K-dwarfs (4200 K), the posteriors are highly asymmetric due to stalled
spin-down, and $\pm$1$\sigma$ age uncertainties vary non-monotonically between
10% and 50% over the first few gigayears. High-mass K-dwarfs (5000 K) older
than 1.5 Gyr yield the most precise ages, with limiting uncertainties currently
set by possible changes in the spin-down rate (12% systematic), the calibration
of the absolute age scale (8% systematic), and the width of the slow sequence
(4% statistical). An open-source implementation, called gyro-interp, is
available online at https://github.com/lgbouma/gyro-interp

Click here to read this post out
ID: 3; Unique Viewers: 0
Unique Voters: 0
Total Votes: 0
Votes:
Latest Change: March 17, 2023, 7:32 a.m. Changes:
Dictionaries:
Words:
Spaces:
Views: 786
CC:
No creative common's license
Comments: