Magnitudes and Other Logarithmic Units¶
Magnitudes and logarithmic units such as dex
and dB
are used as the
logarithm of values relative to some reference value. Quantities with such
units are supported in astropy
via the Magnitude
,
Dex
, and Decibel
classes.
Creating Logarithmic Quantities¶
You can create logarithmic quantities either directly or by multiplication with a logarithmic unit.
Example¶
To create a logarithmic quantity:
>>> import astropy.units as u, astropy.constants as c, numpy as np
>>> u.Magnitude(-10.)
<Magnitude -10. mag>
>>> u.Magnitude(10 * u.ct / u.s)
<Magnitude -2.5 mag(ct / s)>
>>> u.Magnitude(-2.5, "mag(ct/s)")
<Magnitude -2.5 mag(ct / s)>
>>> -2.5 * u.mag(u.ct / u.s)
<Magnitude -2.5 mag(ct / s)>
>>> u.Dex((c.G * u.M_sun / u.R_sun**2).cgs)
<Dex 4.438067627303133 dex(cm / s2)>
>>> np.linspace(2., 5., 7) * u.Unit("dex(cm/s2)")
<Dex [2. , 2.5, 3. , 3.5, 4. , 4.5, 5. ] dex(cm / s2)>
Above, we make use of the fact that the units mag
, dex
, and
dB
are special in that, when used as functions, they return a
LogUnit
instance
(MagUnit
,
DexUnit
, and
DecibelUnit
,
respectively). The same happens as required when strings are parsed
by Unit
.
As for normal Quantity
objects, you can access the value with the
value
attribute. In addition, you can convert to a
Quantity
with the physical unit using the
physical
attribute:
>>> logg = 5. * u.dex(u.cm / u.s**2)
>>> logg.value
5.0
>>> logg.physical
<Quantity 100000. cm / s2>
Converting to Different Units¶
Like Quantity
objects, logarithmic quantities can be converted to different
units, be it another logarithmic unit or a physical one.
Example¶
To convert a logarithmic quantity to a different unit:
>>> logg = 5. * u.dex(u.cm / u.s**2)
>>> logg.to(u.m / u.s**2)
<Quantity 1000. m / s2>
>>> logg.to('dex(m/s2)')
<Dex 3. dex(m / s2)>
For convenience, the si
and
cgs
attributes can be used to
convert the Quantity
to base SI or CGS
units:
>>> logg.si
<Dex 3. dex(m / s2)>
Arithmetic and Photometric Applications¶
Addition and subtraction work as expected for logarithmic quantities, multiplying and dividing the physical units as appropriate. It may be best seen through an example of a photometric reduction.
Example¶
First, calculate instrumental magnitudes assuming some count rates for three objects:
>>> tint = 1000.*u.s
>>> cr_b = ([3000., 100., 15.] * u.ct) / tint
>>> cr_v = ([4000., 90., 25.] * u.ct) / tint
>>> b_i, v_i = u.Magnitude(cr_b), u.Magnitude(cr_v)
>>> b_i, v_i
(<Magnitude [-1.19280314, 2.5 , 4.55977185] mag(ct / s)>,
<Magnitude [-1.50514998, 2.61439373, 4.00514998] mag(ct / s)>)
Then, the instrumental B-V color is:
>>> b_i - v_i
<Magnitude [ 0.31234684, -0.11439373, 0.55462187] mag>
Note that the physical unit has become dimensionless. The following step might be used to correct for atmospheric extinction:
>>> atm_ext_b, atm_ext_v = 0.12 * u.mag, 0.08 * u.mag
>>> secz = 1./np.cos(45 * u.deg)
>>> b_i0 = b_i - atm_ext_b * secz
>>> v_i0 = v_i - atm_ext_b * secz
>>> b_i0, v_i0
(<Magnitude [-1.36250876, 2.33029437, 4.39006622] mag(ct / s)>,
<Magnitude [-1.67485561, 2.4446881 , 3.83544435] mag(ct / s)>)
Since the extinction is dimensionless, the units do not change. Now suppose the first star has a known ST magnitude, so we can calculate zero points:
>>> b_ref, v_ref = 17.2 * u.STmag, 17.0 * u.STmag
>>> b_ref, v_ref
(<Magnitude 17.2 mag(ST)>, <Magnitude 17. mag(ST)>)
>>> zp_b, zp_v = b_ref - b_i0[0], v_ref - v_i0[0]
>>> zp_b, zp_v
(<Magnitude 18.56250876 mag(s ST / ct)>,
<Magnitude 18.67485561 mag(s ST / ct)>)
Here, ST
is shorthand for the ST zero-point flux:
>>> (0. * u.STmag).to(u.erg/u.s/u.cm**2/u.AA)
<Quantity 3.63078055e-09 erg / (Angstrom cm2 s)>
>>> (-21.1 * u.STmag).to(u.erg/u.s/u.cm**2/u.AA)
<Quantity 1. erg / (Angstrom cm2 s)>
Note
At present, only magnitudes defined in terms of luminosity or flux are implemented, since those do not depend on the filter with which the measurement was made. They include absolute and apparent bolometric [M15], ST [H95], and AB [OG83] magnitudes.
Now applying the calibration, we find (note the proper change in units):
>>> B, V = b_i0 + zp_b, v_i0 + zp_v
>>> B, V
(<Magnitude [17.2 , 20.89280314, 22.95257499] mag(ST)>,
<Magnitude [17. , 21.1195437 , 22.51029996] mag(ST)>)
We could convert these magnitudes to another system, for example, ABMag, using appropriate equivalency:
>>> V.to(u.ABmag, u.spectral_density(5500.*u.AA))
<Magnitude [16.99023831, 21.10978201, 22.50053827] mag(AB)>
This is particularly useful for converting magnitude into flux density. V
is currently in ST magnitudes, which is based on flux densities per unit
wavelength (\(f_\lambda\)). Therefore, we can directly convert V
into
flux density per unit wavelength using the
to()
method:
>>> flam = V.to(u.erg/u.s/u.cm**2/u.AA)
>>> flam
<Quantity [5.75439937e-16, 1.29473986e-17, 3.59649961e-18] erg / (Angstrom cm2 s)>
To convert V
to flux density per unit frequency (\(f_\nu\)), we again
need the appropriate equivalency, which in this case
is the central wavelength of the magnitude band, 5500 Angstroms:
>>> lam = 5500 * u.AA
>>> fnu = V.to(u.erg/u.s/u.cm**2/u.Hz, u.spectral_density(lam))
>>> fnu
<Quantity [5.80636959e-27, 1.30643316e-28, 3.62898099e-29] erg / (cm2 Hz s)>
We could have used the central frequency instead:
>>> nu = 5.45077196e+14 * u.Hz
>>> fnu = V.to(u.erg/u.s/u.cm**2/u.Hz, u.spectral_density(nu))
>>> fnu
<Quantity [5.80636959e-27, 1.30643316e-28, 3.62898099e-29] erg / (cm2 Hz s)>
Note
When converting magnitudes to flux densities, the order of operations
matters; the value of the unit needs to be established before the
conversion. For example, 21 * u.ABmag.to(u.erg/u.s/u.cm**2/u.Hz)
will
give you 21 times \(f_\nu\) for an AB mag of 1, whereas (21 *
u.ABmag).to(u.erg/u.s/u.cm**2/u.Hz)
will give you \(f_\nu\) for an AB
mag of 21.
Suppose we also knew the intrinsic color of the first star, then we can calculate the reddening:
>>> B_V0 = -0.2 * u.mag
>>> EB_V = (B - V)[0] - B_V0
>>> R_V = 3.1
>>> A_V = R_V * EB_V
>>> A_B = (R_V+1) * EB_V
>>> EB_V, A_V, A_B
(<Magnitude 0.4 mag>, <Magnitude 1.24 mag>, <Magnitude 1.64 mag>)
Here, you see that the extinctions have been converted to quantities. This
happens generally for division and multiplication, since these processes
work only for dimensionless magnitudes (otherwise, the physical unit would have
to be raised to some power), and Quantity
objects, unlike logarithmic
quantities, allow units like mag / d
.
Note that you can take the automatic unit conversion quite far (perhaps too far, but it is fun). For instance, suppose we also knew the bolometric correction and absolute bolometric magnitude, then we can calculate the distance modulus:
>>> BC_V = -0.3 * (u.m_bol - u.STmag)
>>> M_bol = 5.46 * u.M_bol
>>> DM = V[0] - A_V + BC_V - M_bol
>>> BC_V, M_bol, DM
(<Magnitude -0.3 mag(bol / ST)>,
<Magnitude 5.46 mag(Bol)>,
<Magnitude 10. mag(bol / Bol)>)
With a proper equivalency, we can also convert to
distance without remembering the 5-5log rule (but you might find the
Distance
class to be even more convenient):
>>> radius_and_inverse_area = [(u.pc, u.pc**-2,
... lambda x: 1./(4.*np.pi*x**2),
... lambda x: np.sqrt(1./(4.*np.pi*x)))]
>>> DM.to(u.pc, equivalencies=radius_and_inverse_area)
<Quantity 1000. pc>
NumPy Functions¶
For logarithmic quantities, most numpy
functions and many array methods do
not make sense, hence they are disabled. But you can use those you would expect
to work:
>>> np.max(v_i)
<Magnitude 4.00514998 mag(ct / s)>
>>> np.std(v_i)
<Magnitude 2.33971149 mag>
Note
This is implemented by having a list of supported ufuncs in
units/function/core.py
and by explicitly disabling some array methods in
FunctionQuantity
. If you believe a
function or method is incorrectly treated, please let us know.
Dimensionless Logarithmic Quantities¶
Dimensionless quantities are treated somewhat specially in that, if needed,
logarithmic quantities will be converted to normal Quantity
objects with the
appropriate unit of mag
, dB
, or dex
. With this, it is possible to
use composite units like mag/d
or dB/m
, which cannot conveniently be
supported as logarithmic units. For instance:
>>> dBm = u.dB(u.mW)
>>> signal_in, signal_out = 100. * dBm, 50 * dBm
>>> cable_loss = (signal_in - signal_out) / (100. * u.m)
>>> signal_in, signal_out, cable_loss
(<Decibel 100. dB(mW)>, <Decibel 50. dB(mW)>, <Quantity 0.5 dB / m>)
>>> better_cable_loss = 0.2 * u.dB / u.m
>>> signal_in - better_cable_loss * 100. * u.m
<Decibel 80. dB(mW)>
References
Mamajek et al., 2015, arXiv:1510.06262
E.g., Holtzman et al., 1995, PASP 107, 1065
Oke, J.B., & Gunn, J. E., 1983, ApJ 266, 713