語系:
繁體中文
English
說明(常見問題)
回圖書館首頁
手機版館藏查詢
登入
回首頁
切換:
標籤
|
MARC模式
|
ISBD
Mass distribution of hot stellar sys...
~
Wu, Xiaoan.
FindBook
Google Book
Amazon
博客來
Mass distribution of hot stellar systems.
紀錄類型:
書目-語言資料,印刷品 : Monograph/item
正題名/作者:
Mass distribution of hot stellar systems./
作者:
Wu, Xiaoan.
面頁冊數:
110 p.
附註:
Adviser: Scott Tremaine.
Contained By:
Dissertation Abstracts International68-03B.
標題:
Physics, Astronomy and Astrophysics. -
電子資源:
http://pqdd.sinica.edu.tw/twdaoapp/servlet/advanced?query=3255851
Mass distribution of hot stellar systems.
Wu, Xiaoan.
Mass distribution of hot stellar systems.
- 110 p.
Adviser: Scott Tremaine.
Thesis (Ph.D.)--Princeton University, 2007.
The mass distribution of hot stellar systems is hard to measure because they do not contain gas or star disks, and because there is a degeneracy between the overall mass distribution and the distribution function of the observable particles. Assuming that the potential is spherical, we describe a maximum-likelihood nonparametric method to utilize to the full extent available kinematic data, which is applied to an elliptical galaxy (M87), three dwarf spheroidal galaxies (Draco, Ursa Minor and Fornax) and a globular cluster (o Centauri). For M87, the mass within 32 kpc is (2:4 +/- 0:6) x 1012 M ⊙ , and the exponent of the density profile rho ∝ r -alpha in the range 10 - 100 kpc is alpha = 1:6 +/- 0:4. The energy distribution suggests a few kinematically distinct groups of globular clusters. For dwarf spheroidal galaxies, our models naturally produce the so-called "extra-tidal extensions", which had previously been suggested as evidence of tidal stripping. The average V-band mass-to-light ratio is 400 +/- 80M ⊙ =LV, ⊙ within 0:75 kpc for Draco, 580+140-100 M ⊙ =V, ⊙ within 1:1 kpc for Ursa Minor and 25+7-5 M ⊙ =LV, ⊙ within 2:5 kpc for Fornax. We do not find that anisotropy contributes substantially to the high mass-to-light ratios in these dSph galaxies. For o Centauri, we derive an averaged (V -band) mass-to-light ratio Gamma = 2:96 +/- 0:10 M ⊙/L ⊙ . Moreover, we find no evidence that the even part of the DF is dependent on total angular momentum; that is, two-integral models in which the DF depends on energy and the z'-component of angular momentum are sufficient to fit the data.Subjects--Topical Terms:
1019521
Physics, Astronomy and Astrophysics.
Mass distribution of hot stellar systems.
LDR
:02465nam 2200253 a 45
001
954244
005
20110621
008
110622s2007 eng d
035
$a
(UMI)AAI3255851
035
$a
AAI3255851
040
$a
UMI
$c
UMI
100
1
$a
Wu, Xiaoan.
$3
1277717
245
1 0
$a
Mass distribution of hot stellar systems.
300
$a
110 p.
500
$a
Adviser: Scott Tremaine.
500
$a
Source: Dissertation Abstracts International, Volume: 68-03, Section: B, page: 1682.
502
$a
Thesis (Ph.D.)--Princeton University, 2007.
520
$a
The mass distribution of hot stellar systems is hard to measure because they do not contain gas or star disks, and because there is a degeneracy between the overall mass distribution and the distribution function of the observable particles. Assuming that the potential is spherical, we describe a maximum-likelihood nonparametric method to utilize to the full extent available kinematic data, which is applied to an elliptical galaxy (M87), three dwarf spheroidal galaxies (Draco, Ursa Minor and Fornax) and a globular cluster (o Centauri). For M87, the mass within 32 kpc is (2:4 +/- 0:6) x 1012 M ⊙ , and the exponent of the density profile rho ∝ r -alpha in the range 10 - 100 kpc is alpha = 1:6 +/- 0:4. The energy distribution suggests a few kinematically distinct groups of globular clusters. For dwarf spheroidal galaxies, our models naturally produce the so-called "extra-tidal extensions", which had previously been suggested as evidence of tidal stripping. The average V-band mass-to-light ratio is 400 +/- 80M ⊙ =LV, ⊙ within 0:75 kpc for Draco, 580+140-100 M ⊙ =V, ⊙ within 1:1 kpc for Ursa Minor and 25+7-5 M ⊙ =LV, ⊙ within 2:5 kpc for Fornax. We do not find that anisotropy contributes substantially to the high mass-to-light ratios in these dSph galaxies. For o Centauri, we derive an averaged (V -band) mass-to-light ratio Gamma = 2:96 +/- 0:10 M ⊙/L ⊙ . Moreover, we find no evidence that the even part of the DF is dependent on total angular momentum; that is, two-integral models in which the DF depends on energy and the z'-component of angular momentum are sufficient to fit the data.
590
$a
School code: 0181.
650
4
$a
Physics, Astronomy and Astrophysics.
$3
1019521
690
$a
0606
710
2
$a
Princeton University.
$3
645579
773
0
$t
Dissertation Abstracts International
$g
68-03B.
790
$a
0181
790
1 0
$a
Tremaine, Scott,
$e
advisor
791
$a
Ph.D.
792
$a
2007
856
4 0
$u
http://pqdd.sinica.edu.tw/twdaoapp/servlet/advanced?query=3255851
筆 0 讀者評論
館藏地:
全部
電子資源
出版年:
卷號:
館藏
1 筆 • 頁數 1 •
1
條碼號
典藏地名稱
館藏流通類別
資料類型
索書號
使用類型
借閱狀態
預約狀態
備註欄
附件
W9118723
電子資源
11.線上閱覽_V
電子書
EB W9118723
一般使用(Normal)
在架
0
1 筆 • 頁數 1 •
1
多媒體
評論
新增評論
分享你的心得
Export
取書館
處理中
...
變更密碼
登入