Commit 46a274688648367ea2d32fe7c84f1ca8bb3bd074
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Update IRF section of User Manual
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doc/source/users/user_manual/irfs.jpg
100755 → 100644
doc/source/users/user_manual/likelihood.rst
| ... | ... | @@ -210,7 +210,7 @@ Model fitting using the Levenberg-Marquardt algorithm is implemented by |
| 210 | 210 | :ref:`ctlike`. |
| 211 | 211 | |
| 212 | 212 | |
| 213 | -Statistical Parameter errors | |
| 213 | +Statistical parameter errors | |
| 214 | 214 | ~~~~~~~~~~~~~~~~~~~~~~~~~~~~ |
| 215 | 215 | |
| 216 | 216 | Statistical errors on the model parameters :math:`\delta a_k` are determined |
| ... | ... | @@ -256,8 +256,8 @@ fluctuations only. For :math:`n=1` the significance in Gaussian sigma |
| 256 | 256 | is given by :math:`\sqrt{TS}`. |
| 257 | 257 | |
| 258 | 258 | |
| 259 | -Upper limits | |
| 260 | -~~~~~~~~~~~~ | |
| 259 | +Upper flux limits | |
| 260 | +~~~~~~~~~~~~~~~~~ | |
| 261 | 261 | |
| 262 | 262 | If gamma-ray emission from a source is not detected, an upper flux limit can |
| 263 | 263 | be derived by determining the flux :math:`F_\mathrm{up}` that leads to a | ... | ... |
doc/source/users/user_manual/response.rst
| ... | ... | @@ -7,40 +7,32 @@ What are instrument response functions? |
| 7 | 7 | ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ |
| 8 | 8 | |
| 9 | 9 | The instrument response functions provide a mathematical description that |
| 10 | -links the measured quantities :math:`\vec{d}` of an event to the physical | |
| 11 | -quantities :math:`\vec{p}` of the incident photon. The following figure | |
| 12 | -illustrates this relationship: | |
| 10 | +links the reconstructed photon arrival direction :math:`p'`, energy :math:`E'` | |
| 11 | +and trigger time :math:`t'` of an event to the true incident direction | |
| 12 | +:math:`p`, energy :math:`E` and time :math:`t` of a photon. The following | |
| 13 | +figure illustrates this relationship: | |
| 13 | 14 | |
| 14 | 15 | .. figure:: irfs.jpg |
| 15 | 16 | :width: 70% |
| 16 | 17 | |
| 17 | -:math:`I(\vec{p})` is the gamma-ray intensity arriving at Earth as a | |
| 18 | -function of photon properties :math:`\vec{p}` | |
| 19 | -(which usually are true photon energy, true photon incident direction, | |
| 20 | -and true photon arrival time), | |
| 21 | -while :math:`e(\vec{d})` is the expected event rate as function of event | |
| 22 | -properties :math:`\vec{d}` (which usually are the measured photon energy, | |
| 23 | -measured or reconstructued photon incident direction, and measured photon | |
| 24 | -arrival time). The expected event rate is obtained by integrating the | |
| 25 | -product of | |
| 26 | -the instrumental response function :math:`R(\vec{d}|\vec{p},\vec{a}`) | |
| 27 | -and the emitted intensity :math:`I(\vec{p})` over the photon properties | |
| 28 | -:math:`\vec{p}`. | |
| 29 | -The argument :math:`\vec{a}` in the response function comprises any | |
| 30 | -auxiliary parameter on which the response function may depend on (e.g. | |
| 31 | -pointing direction, triggered telescopes, optical efficiencies, | |
| 32 | -atmospheric conditions, etc.). All these quantities and hence the | |
| 33 | -instrument response function may depend on time. | |
| 18 | +:math:`I(p,E,t)` is the gamma-ray intensity arriving at Earth as a function of | |
| 19 | +direction :math:`p`, energy :math:`E` and time :math:`t`. :math:`e(p',E',t')` | |
| 20 | +is the expected event rate as function of the reconstructed direction | |
| 21 | +:math:`p'`, energy :math:`E'` and trigger time :math:`t'`. The expected event | |
| 22 | +rate is obtained by integrating the product of the instrumental response | |
| 23 | +function :math:`R(p',E',t'|p,E,t)` and the emitted intensity :math:`I(p,E,t)` | |
| 24 | +over the direction, energy and time. | |
| 34 | 25 | |
| 35 | 26 | |
| 36 | 27 | CTA response functions |
| 37 | 28 | ~~~~~~~~~~~~~~~~~~~~~~ |
| 38 | 29 | |
| 39 | -The instrument response functions for CTA are factorised into | |
| 30 | +The instrument response functions for CTA (as well as the other IACTs such as | |
| 31 | +H.E.S.S., VERITAS and MAGIC) are factorised into | |
| 40 | 32 | the effective area :math:`A_{\rm eff}(p, E, t)` (units :math:`cm^2`), |
| 41 | 33 | the point spread function :math:`PSF(p' | p, E, t)`, |
| 42 | 34 | and the energy dispersion :math:`E_{\rm disp}(E' | p, E, t)` |
| 43 | -following: | |
| 35 | +following | |
| 44 | 36 | |
| 45 | 37 | .. math:: |
| 46 | 38 | R(p', E', t' | p, E, t) = |
| ... | ... | @@ -48,7 +40,17 @@ following: |
| 48 | 40 | PSF(p' | p, E, t) \times |
| 49 | 41 | E_{\rm disp}(E' | p, E, t) |
| 50 | 42 | |
| 51 | -ctools are shipped with so called ``prod2`` response functions for the northern | |
| 43 | +where | |
| 44 | + | |
| 45 | +.. math:: | |
| 46 | + \int PSF(p' | p, E, t) dp' = 1 | |
| 47 | + | |
| 48 | +and | |
| 49 | + | |
| 50 | +.. math:: | |
| 51 | + \int E_{\rm disp}(E' | p, E, t) dE' = 1 | |
| 52 | + | |
| 53 | +ctools are shipped with the CTA ``prod2`` response functions for the northern | |
| 52 | 54 | and southern arrays, and variants are available that have been optimised for |
| 53 | 55 | exposure times of 0.5 hours, 5 hours and 50 hours. |
| 54 | 56 | In total, the following six instrument response functions are available: |
| ... | ... | @@ -56,9 +58,9 @@ In total, the following six instrument response functions are available: |
| 56 | 58 | ``South_5h``, and ``South_50h``. |
| 57 | 59 | |
| 58 | 60 | .. note:: |
| 59 | - In cases for which the CTA instrument response functions are used in a | |
| 60 | - research project, we ask to add the following acknowledgement in any | |
| 61 | - resulting publication: | |
| 61 | + If you use the CTA instrument response functions for a research project | |
| 62 | + and specifically for a presentation or publication, we ask to add the | |
| 63 | + following acknowledgement to the presentation or publication: | |
| 62 | 64 | |
| 63 | 65 | *This research has made use of the CTA instrument response functions |
| 64 | 66 | provided by the CTA Consortium and Observatory.* | ... | ... |