![[EXT]](images/offsite.png)
Transformations between SDSS magnitudes and other systems
Introduction
There have been several efforts to calculate transformations between ugriz (or u'g'r'i'z') and UBVRcIc. Here, we summarize seven such efforts. We note that any such transformation relies on knowledge of the absolute calibration, and is inherently uncertain.
Jump to:
- Jester et al. (2005)
- Jordi et al. (2006)
- Karaali, Bilir & Tunçel (2005)
- Bilir, Karaali & Tunçel (2005)
- West, Walkowicz & Hawley (2005)
- Rodgers et al. (2006)
- Lupton (2005)
Note that Jester et al. (2005) derived transformation equations for stars and for z <= 2.1 quasars; Jordi et al. (2006), for stars, including those for Population I and metal-poor Population II stars; Karaali et al. (2005), for stars; Bilir et al. (2005), for dwarf stars, West et al. (2005), for M and L dwarf stars, Rodgers et al. (2006), for main sequence stars; and Lupton (2005), for stars.
There are currently no transformation equations explicitly for galaxies, but Jester et al.'s (2005) and Lupton's (2005) transformation equations for stars should also provide reasonable results for normal galaxies (i.e., galaxies without strong emission lines).
Caveat: Note that these transformation equations are for the SDSS ugriz (u'g'r'i'z') magnitudes as measured, not for SDSS ugriz (u'g'r'i'z') corrected for AB offsets. If you need AB ugriz magnitudes, please remember to convert from SDSS ugriz to AB ugriz using AB offsets described here).
Jester et al. (2005)
The following transformation equations were extracted from Table 1 of Jester et al. (2005) and are generally useful for stars and for quasars. The transformation equations for z <= 2.1 quasars is based upon synthetic photometry of an updated version of the quasar composite spectrum of Vanden Berk et al. (2001) using DR1 data as well as the red and reddened quasar composites for Richards et al. (2003). The transformations for stars were derived from the Smith et al. (2002) u'g'r'i'z' photometry of Landolt stars, suitably transformed from the USNO-1.0m u'g'r'i'z' system to the SDSS 2.5m ugriz system via the u'g'r'i'z'-to-ugriz transformations.
The transformation equations for stars supercede those of Fukugita et al. (1996) and Smith et al. (2002).
UBVRcIc -> ugriz
================
Quasars at z <= 2.1 (synthetic)
Transformation RMS residual
u-g = 1.25*(U-B) + 1.02 0.03
g-r = 0.93*(B-V) - 0.06 0.09
r-i = 0.90*(Rc-Ic) - 0.20 0.07
r-z = 1.20*(Rc-Ic) - 0.20 0.18
g = V + 0.74*(B-V) - 0.07 0.02
r = V - 0.19*(B-V) - 0.02 0.08
Stars with Rc-Ic < 1.15 and U-B < 0
Transformation RMS residual
u-g = 1.28*(U-B) + 1.14 0.05
g-r = 1.09*(B-V) - 0.23 0.04
r-i = 0.98*(Rc-Ic) - 0.22 0.01
r-z = 1.69*(Rc-Ic) - 0.42 0.03
g = V + 0.64*(B-V) - 0.13 0.01
r = V - 0.46*(B-V) + 0.11 0.03
All stars with Rc-Ic < 1.15
Transformation RMS residual
u-g = 1.28*(U-B) + 1.13 0.06
g-r = 1.02*(B-V) - 0.22 0.04
r-i = 0.91*(Rc-Ic) - 0.20 0.03
r-z = 1.72*(Rc-Ic) - 0.41 0.03
g = V + 0.60*(B-V) - 0.12 0.02
r = V - 0.42*(B-V) + 0.11 0.03
ugriz -> UBVRcIc
================
Quasars at z <= 2.1 (synthetic)
Transformation RMS residual
U-B = 0.75*(u-g) - 0.81 0.03
B-V = 0.62*(g-r) + 0.15 0.07
V-R = 0.38*(r-i) + 0.27 0.09
Rc-Ic = 0.72*(r-i) + 0.27 0.06
B = g + 0.17*(u-g) + 0.11 0.03
V = g - 0.52*(g-r) - 0.03 0.05
Stars with Rc-Ic < 1.15 and U-B < 0
Transformation RMS residual
U-B = 0.77*(u-g) - 0.88 0.04
B-V = 0.90*(g-r) + 0.21 0.03
V-R = 0.96*(r-i) + 0.21 0.02
Rc-Ic = 1.02*(r-i) + 0.21 0.01
B = g + 0.33*(g-r) + 0.20 0.02
V = g - 0.58*(g-r) - 0.01 0.02
All stars with Rc-Ic < 1.15
Transformation RMS residual
U-B = 0.78*(u-g) - 0.88 0.05
B-V = 0.98*(g-r) + 0.22 0.04
V-R = 1.09*(r-i) + 0.22 0.03
Rc-Ic = 1.00*(r-i) + 0.21 0.01
B = g + 0.39*(g-r) + 0.21 0.03
V = g - 0.59*(g-r) - 0.01 0.01
Jordi et al. (2005)
The following transformation equations were extracted from Table 3 of Jordi et al. (2006) and are generally useful for stars. They are derived from comparing Stetson's extension of the Landolt standard stars with the corresponding SDSS DR4 photometry. The equations including the Johnson U band are based on the comparison of Landolt's original standard stars and the SDSS DR4.
UBVRcIc -> ugriz
================
Transformation
u-g = (0.750 ± 0.050)*(U-B) + (0.770 ± 0.070)*(B-V) + (0.720 ± 0.040)
g-V = (0.630 ± 0.002)*(B-V) - (0.124 ± 0.002)
g-B = (-0.370 ± 0.002)*(B-V) - (0.124 ± 0.002)
g-r = (1.646 ± 0.008)*(V-R) - (0.139 ± 0.004)
g-i = (1.481 ± 0.004)*(V-I) - (0.536 ± 0.004) if V-I <= 1.8
g-i = (0.83 ± 0.01)*(V-I) + (0.60 ± 0.03) if V-I > 1.8
r-i = (1.007 ± 0.005)*(R-I) - (0.236 ± 0.003)
r-z = (1.584 ± 0.008)*(R-I) - (0.386 ± 0.005)
r-R = (0.267 ± 0.005)*(V-R) + (0.088 ± 0.003) if V-R <= 0.93
r-R = (0.77 ± 0.04)*(V-R) - (0.37 ± 0.04) if V-R > 0.93
i-I = (0.247 ± 0.003)*(R-I) + (0.329 ± 0.002)
ugriz -> UBVRcIc
================
Transformation
U-B = (0.79 ± 0.02)*(u-g) - (0.93 ± 0.02)
U-B = (0.52 ± 0.06)*(u-g) + (0.53 ± 0.09)*(g-r) - (0.82 ± 0.04)
B-g = (0.175 ± 0.002)*(u-g) + (0.150 ± 0.003)
B-g = (0.313 ± 0.003)*(g-r) + (0.219 ± 0.002)
V-g = (-0.565 ± 0.001)*(g-r) - (0.016 ± 0.001)
V-I = (0.675 ± 0.002)*(g-i) + (0.364 ± 0.002) if g-i <= 2.1
V-I = (1.11 ± 0.02)*(g-i) - (0.52 ± 0.05) if g-i > 2.1
R-r = (-0.153 ± 0.003)*(r-i) - (0.117 ± 0.003)
R-I = (0.930 ± 0.005)*(r-i) + (0.259 ± 0.002)
I-i = (-0.386 ± 0.004)*(i-z) - (0.397 ± 0.001)
The following transformation equations were extracted from Table 4 of Jordi et al. (2006) and are generally useful for Population I and metal-poor Population II stars, respectively. The transformations for the Population II stars are derived from comparing Stetson fields around Draco, NGC 2419 and NGC 7078 with their SDSS DR4 photometry. The transformations for the Population I stars are derived from the Stetson extension of Landolt's equatorial fields compared with the SDSS DR4 photometry. The transformation equation for Population II stars including the SDSS (i-z)-color is not calculated, because of the small number of stars.
BVRcIc -> griz
================
Transformation for Population I stars:
g-V = (0.634 ± 0.002)*(B-V) - (0.127 ± 0.002)
g-B = (-0.366 ± 0.002)*(B-V) - (0.126 ± 0.002)
g-r = (1.599 ± 0.009)*(V-R) - (0.106 ± 0.006)
g-i = (1.474 ± 0.004)*(V-I) - (0.518 ± 0.005) if V-I <= 1.8
g-i = (0.83 ± 0.01)*(V-I) + (0.62 ± 0.03) if V-I > 1.8
r-i = (0.988 ± 0.006)*(R-I) - (0.221 ± 0.004)
r-z = (1.568 ± 0.009)*(R-I) - (0.370 ± 0.006)
r-R = (0.275 ± 0.006)*(V-R) + (0.086 ± 0.004) if V-R <= 0.93
r-R = (0.71 ± 0.05)*(V-R) - (0.31 ± 0.05) if V-R > 0.93
i-I = (0.251 ± 0.003)*(R-I) + (0.325 ± 0.002)
Transformation for metal-poor Population II stars:
g-V = (0.596 ± 0.009)*(B-V) - (0.148 ± 0.007)
g-B = (-0.401 ± 0.009)*(B-V) - (0.145 ± 0.006)
g-r = (1.72 ± 0.02)*(V-R) - (0.198 ± 0.007)
g-i = (1.48 ± 0.01)*(V-I) - (0.57 ± 0.01) if V-I <= 1.8
r-i = (1.06 ± 0.02)*(R-I) - (0.30 ± 0.01)
r-z = (1.60 ± 0.06)*(R-I) - (0.46 ± 0.03)
r-R = (0.34 ± 0.02)*(V-R) + (0.015 ± 0.008) if V-R <= 0.93
i-I = (0.21 ± 0.02)*(R-I) + (0.34 ± 0.01)
griz -> BVRcIc
================
Transformation for Population I stars:
B-g = (0.163 ± 0.002)*(u-g) + (0.170 ± 0.004)
B-g = (0.312 ± 0.003)*(g-r) + (0.219 ± 0.002)
V-g = (-0.573 ± 0.002)*(g-r) - (0.016 ± 0.002)
V-I = (0.671 ± 0.002)*(g-i) + (0.359 ± 0.002) if g-i <= 2.1
V-I = (1.12 ± 0.02)*(g-i) - (0.53 ± 0.06) if g-i > 2.1
R-r = (-0.257 ± 0.004)*(r-i) + (0.152 ± 0.002)
R-I = (0.977 ± 0.006)*(r-i) + (0.234 ± 0.003)
I-i = (-0.409 ± 0.006)*(i-z) - (0.394 ± 0.002)
Transformation for metal-poor Population II stars:
B-g = (0.20 ± 0.01)*(u-g) + (0.15 ± 0.01)
B-g = (0.349 ± 0.009)*(g-r) + (0.245 ± 0.006)
V-g = (-0.569 ± 0.007)*(g-r) + (0.021 ± 0.004)
V-I = (0.674 ± 0.005)*(g-i) + (0.406 ± 0.004) if g-i <= 2.1
R-r = (-0.25 ± 0.02)*(r-i) - (0.119 ± 0.005)
R-I = (0.80 ± 0.02)*(r-i) + (0.317 ± 0.004)
Karaali, Bilir & Tunçel (2005)
These transformations appeared in Karaali, Bilir & Tunçel (2005). They are based on Landolt (1992) UBV data for 224 stars in the color range 0.3 < B-V < 1.1 with SDSS ugr photometry from the CASU INT Wide Field Survey. An improvement over previous SDSS - UBVRcIc transformations is the use of two colors in each equation, which is particularly helpful for the u-g transformation.
UBVRcIc -> ugriz
================
Stars with 0.3 < B-V < 1.1
u-g = 0.779*(U-B) + 0.755*(B-V) + 0.801
g-r = 1.023*(B-V) + 0.016*(U-B) - 0.187
ugriz -> UBVRcIc
================
Stars with 0.3 < B-V < 1.1
B-V = 0.992*(g-r) - 0.0199*(u-g) + 0.202
Bilir, Karaali & Tunçel (2005)
These transformation equations appeared in Bilir, Karaali & Tunçel (2005). They are based upon 195 dwarf stars that have both ugriz photometry and Landolt UBV photometry.
UBVRcIc -> ugriz
================
Dwarf (Main Sequence) Stars
g-r = 1.124*(B-V) - 0.252
r-i = 1.040*(R-I) - 0.224
g = V + 0.634*(B-V) - 0.108
West, Walkowicz & Hawley (2005)
These transformation equations appeared in West, Walkowicz & Hawley (2005). They are based upon photometry of M and L dwarf stars from SDSS Data Release 3.
UBVRcIc -> ugriz
================
M0-L0 Dwarfs, 0.67 <= r-i <= 2.01
Transformation RMS residual
r-i = -2.69 + 2.29*(V-Ic) 0.05
- 0.28*(V-Ic)**2
M0-L0 Dwarfs, 0.37 <= i-z <= 1.84
Transformation RMS residual
i-z = -20.6 + 26.0*(Ic-Ks) 0.10
- 11.7*(Ic-Ks)**2
- 2.30*(Ic-Ks)**3
- 0.17*(Ic-Ks)**4
Rodgers et al. (2006)
These equations are from Rodgers et al. (2006). They are based upon a set of main sequence stars from the Smith et al. (2002) u'g'r'i'z' standard star network that also have Landolt UBVRcIc photometry. Note that these equations, strictly speaking, transform from UBVRcIc to u'g'r'i'z' and not to ugriz. The transformation from u'g'r'i'z' to ugriz, however, is rather small. Note also, as with the Karaali, Bilir & Tunçel (2005) transformations listed above, two colors are used in the u'-g' and g'-r' equations to improve the fits. The use of two colors in the fits is especially useful for u'-g', which is strongly affected by the Balmer discontinuity.
UBVRcIc -> u'g'r'i'z'
=====================
Main Sequence Stars
u'-g' = (1.101 ± 0.004)*(U-B) + (0.358 ± 0.004)*(B-V) + 0.971
g'-r' = (0.278 ± 0.016)*(B-V) + (1.321 ± 0.030)*(V-Rc) - 0.219
r'-i' = (1.000 ± 0.006)*(Rc-Ic) - 0.212
r'-z' = (1.567 ± 0.020)*(Rc-Ic) - 0.365
Lupton (2005)
These equations that Robert Lupton derived by matching DR4 photometry to Peter Stetson's published photometry for stars.
Stars B = u - 0.8116*(u - g) + 0.1313; sigma = 0.0095 B = g + 0.3130*(g - r) + 0.2271; sigma = 0.0107 V = g - 0.2906*(u - g) + 0.0885; sigma = 0.0129 V = g - 0.5784*(g - r) - 0.0038; sigma = 0.0054 R = r - 0.1837*(g - r) - 0.0971; sigma = 0.0106 R = r - 0.2936*(r - i) - 0.1439; sigma = 0.0072 I = r - 1.2444*(r - i) - 0.3820; sigma = 0.0078 I = i - 0.3780*(i - z) -0.3974; sigma = 0.0063
Here is the CAS SQL query Robert used to perform the matchup of DR4 photometry with Stetson's:
select
dbo.fSDSS(P.objId) as ID, name,
S.B, S.Berr, S.V, S.Verr , S.R, S.Rerr, S.I, S.Ierr,
psfMag_u, psfMagErr_u, psfMag_g, psfMagErr_g,
psfMag_r, psfMagErr_r, psfMag_i, psfMagErr_i, psfMag_z, psfMagErr_z,
case when 0 = (flags_u & 0x800d00000000000) and status_u = 0 then 1 else 0 end as good_u,
case when 0 = (flags_g & 0x800d00000000000) and status_g = 0 then 1 else 0 end as good_g,
case when 0 = (flags_r & 0x800d00000000000) and status_r = 0 then 1 else 0 end as good_r,
case when 0 = (flags_i & 0x800d00000000000) and status_i = 0 then 1 else 0 end as good_i,
case when 0 = (flags_z & 0x800d00000000000) and status_z = 0 then 1 else 0 end as good_z
from
stetson as S
join star as P on S.objId = P.objId
join field as F on P.fieldId = F.fieldId
where
0 = (flags & 0x40006)