“Bar”的版本间差异
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==pattern speed== |
==pattern speed== |
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defined as the rotational frequency of the bar. |
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* |
* Bar cannot extend beyond the corotation resonance (CR) radius of the galaxy. |
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* CR is the region of the galaxy where the angular speed of the stars of the disc in circular motions equals the bar pattern speed. |
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* This limit is imposed by the stability of the main family of orbits forming the bar (the so-called x1 family; Contopoulos 1980) which are only stable within R(CR). Orbits in the outer region of the disc (R > RCR) |
* This limit is imposed by the stability of the main family of orbits forming the bar (the so-called x1 family; Contopoulos 1980) which are only stable within R(CR). Orbits in the outer region of the disc (R > RCR) cannot support a bar structure. |
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* hypothesis: that fast bars are formed by global instabilities in isolated galaxies, while slow bars are triggered by tidal interactions in dense environments arXiv:2511.02054 |
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==形成机制== |
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* Can A Kinematically Hot and Thick Disk Form A Bar? : Role of Highly Spinning Dark Matter Halos arXiv:2512.21632 |
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:*高红移星系,动力学上更热,看到了棒结构,可能与旋转的晕有关。 |
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2025年12月29日 (一) 10:34的最新版本
- 描述棒星系的三个参数,长度,强度,和pattern speed [1]
strength
The bar strength is a parameter that measures the non-axisymmetric forces produced by the bar potential in the disc of galaxies (see, e.g., Laurikainen & Salo, 2002).
- measure the torques of the bar (e.g., Combes & Sanders , 1981; Quillen et al. , 1994; Buta & Block , 2001; Laurikainen et al. , 2007; Salo et al. , 2010)
- bar ellipticity Martinet & Friedli (1997); Aguerri (1999); Whyte et al. (2002); Marinova & Jogee (2007); Aguerri et al. (2009)
- Fourier decomposition of the galaxy light Ohta et al. (1990); Marquez et al. (1996); Aguerri et al. (2000); Athanassoula & Misiriotis (2002); Laurikainen et al. (2005).
pattern speed
defined as the rotational frequency of the bar.
- Bar cannot extend beyond the corotation resonance (CR) radius of the galaxy.
- CR is the region of the galaxy where the angular speed of the stars of the disc in circular motions equals the bar pattern speed.
- This limit is imposed by the stability of the main family of orbits forming the bar (the so-called x1 family; Contopoulos 1980) which are only stable within R(CR). Orbits in the outer region of the disc (R > RCR) cannot support a bar structure.
- hypothesis: that fast bars are formed by global instabilities in isolated galaxies, while slow bars are triggered by tidal interactions in dense environments arXiv:2511.02054
形成机制
- Can A Kinematically Hot and Thick Disk Form A Bar? : Role of Highly Spinning Dark Matter Halos arXiv:2512.21632
- 高红移星系,动力学上更热,看到了棒结构,可能与旋转的晕有关。