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Table 5

Observationally determined slopes of the L − T relation.

Relation Slope Comments Reference

LX1 − Ta 2.02 ± 0.4 35 clusters ROSAT/ASCA Markevitch98
LX1 − Tb 2.10 ± 0.24 Markevitch98
Lbol − Tb 2.64 ± 0.27 Markevitch98
Lbol − T 2.88 ± 0.27 24 clusters ROSAT/GINGA Arnaud99
LX1 − Tc 2.47 ± 0.14 88 clusters ROSAT/ASCA Ikebe02
Lbol − T 3.72 ± 0.47 28 clusters, z = 0.4−1.3 Ettori04
Lbol − T 2.78 ± 0.55 11 clusters, z = 0.6−1.0 Maughan06
Lbol − Tf 2.80 ± 0.2 115 clusters, z = 0.1−1.3 Maughan07
Lbol − T 2.35 ± 0.33 70 clusters, z = 0.18−1.24 O’Hara07
Lbol − Td 2.26 ± 0.33 O’Hara07
Lbol − T 2.90 ± 0.35 27 RCS & CNOC clusters Hicks08
LX1 − Te 2.13 ± 0.32 37 clusters, XMM-Newton Zhang08
Lbol − Te 2.61 ± 0.32 Zhang08
LX1 − T 2.24 ± 0.22 31 clusters, XMM-Newton Pratt09
Lbol − T 2.70 ± 0.24 Pratt09
LX1 − Tf 2.32 ± 0.13 Pratt09
Lbol − Tf 2.78 ± 0.13 Pratt09
Lbol − T 2.53 ± 0.15 14 literature samples Reichert11

Notes. LX1 is the temperature in the 0.1 to 2.4 keV band, LX2 for the 0.5 to 2 keV band, and Lbol the bolometric luminosity.

(a)

For total luminosity.

(b)

Luminosity and temperature corrected for cool core contribution.

(c)

Temperature was determined by allowing for an additional cool component not considered in the correlation.

(d)

Core excised LX and T with r ≥ 0.2r500.

(e)

Temperatures for r = 0.2−0.5 × r500.

(f)

Core excised L and T with r = 0.15−1 × r500.

References not listed in Table 4 from top to bottom are: Markevitch (1998), Arnaud & Evrard (1999), Ikebe et al. (2002), Maughan (2007), Pratt et al. (2009).

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