Model of space charge(s) and its connection to the photon rate in - - PowerPoint PPT Presentation
Model of space charge(s) and its connection to the photon rate in - - PowerPoint PPT Presentation
Model of space charge(s) and its connection to the photon rate in LArTPC Xiao Luo (Yale, UCSB), Flavio Cavanna (FNAL) ProtoDUNE DRA meeting April 17 th 2019 The origin - ionization charges Electrons are the LArTPC signal, but our model focus the
The origin - ionization charges
Electrons are the LArTPC signal, but our model focus the invisible ions (e.g. Ar2
+)
The story starts with ions (space charges)...
3
z
Ar+ Ar+ Ar+ Ar+ e- e- e- e- e- e- Ar+
Anode Cathode
Ar+
x
E E
Ar2+ Ar2+ Ar2+ Ar2+ Ar2+ Ar2+ Ar2+ Ar2+ Ar2+ Ar2+ Ar2+ Ar2+ Ar2+ Ar2+ Ar2+
Cathode
Anode Large detector, equilibrium
~ hour
Ion transport eq. at equilibrium:
dx Considering the flux
- nly in 1-D
Simplest case – ionization only
0.5 1.0 1.5 2.0 2.5 3.0 3.5 40000 45000 50000 55000 60000 65000 70000
E field Vs X E [V/m] Drift X [m]
0.5 1.0 1.5 2.0 2.5 3.0 3.5 2.0×1011 4.0×1011 6.0×1011 8.0×1011 1.0×1012 1.2×1012
Ar2+ Vs X Drift X [m] n+ [m-3] [EA,EC] = [-25%, +43%]
Parameters:
Cosmic muon rate: 13kHz npair - rate of (e-, I+) pairs after initial recombination: 1.9e9 [m-3s-1]
Ion mobility: 8e-8 [m2V-1s-1] Ion velocity (E=500V/cm): 4e-3 [m/s]
Add e- attachment: e- + X -> X-
Attachment
0.5 1.0 1.5 2.0 2.5 3.0 3.5 1×1011 2×1011 3×1011 4×1011
H2O- Vs X E field Vs X Drift X [m] E [V/m]
Ionization only + Attachement
0.5 1.0 1.5 2.0 2.5 3.0 3.5 40000 45000 50000 55000 60000 65000 70000
e- at attach achmen ment to impu mpurity y (e. (e.g. H2O) O): 𝑓9 + 𝐼<𝑃 → 𝐼<𝑃9
Parameters:
- Atta. (to H2O) Rate: kA [H2O]= 1.4 x 10-15 [m3s-1]
H2O Concentration: c[H2O] = 3ppt Lifetime: 6ms.
Drift X [m] n- [m-3]
Add Mutual Neutralization
Ar2+ Ar2+ Ar2+ Ar2+ Ar2+ Ar2+ Ar2+ Ar2+ Ar2+ Ar2+ Ar2+ Ar2+ Ar2+
Ar2+
O2- O2- O2- O2- O2- O2- O2- O2- O2- O2- O2-
Cathode Anode
New process we incorporate in our model: Mutual Neutralization (MN) 𝐵𝑠
< A + 𝐼<𝑃9 → 𝐵𝑠 < ∗ + 𝐼<𝑃
→ 2𝐵𝑠 + 𝛿 + 𝐼<𝑃 𝑙EF𝑜9𝑜A
Parameters asso. with this process: MN rate constant: kMN = 2.8e-13 [m3/s] Photon generation rate is
Assume each time MN happens, generating 1 VUV photon
Ionization only + Attachement + Mutual Neutralization
0.5 1.0 1.5 2.0 2.5 3.0 3.5 40000 45000 50000 55000 60000 65000 70000
Attachment +Mutual Neutralization
0.5 1.0 1.5 2.0 2.5 3.0 3.5 1×1011 2×1011 3×1011 4×1011
E field Vs X H2O- Vs X Ar2+ Vs X
Ionization only + Attachement + Mutual Neutralization
0.5 1.0 1.5 2.0 2.5 3.0 3.5 2.0×1011 4.0×1011 6.0×1011 8.0×1011 1.0×1012 1.2×1012
𝛿 Vs X
E (V/m) Drift X (m) Drift X (m)
0.5 1.0 1.5 2.0 2.5 3.0 3.5 1×108 2×108 3×108 4×108 5×108 6×108
Mutual Neutralization cont.
𝐽A + 𝐽9 → γ
n+ [m-3] n- [m-3] [m-3 s-1] X[m] X[m] X[m] X[m]
Add the Volume Recombination
New process that we incorporate in our model. Note the difference from the well-known initial recombination process Volume Recombination (VR) 𝐵𝑠
< A + 𝑓9 → 𝐵𝑠 < ∗ → 2𝐵𝑠 + 𝛿
E
Ar2+ Ar2+ Ar2+ Ar2+ Ar2+ Ar2+ Ar2+ Ar2+ Ar2+ Ar2+ Ar2+ Ar2+ Ar2+ Ar2+ Ar2+
Cathode Anode
e-
Parameters asso. with this process: VR rate constant: kR = 1.1e-10 m3/s Photon generation rate is 𝑙J𝑜A𝑜K
Assume each time VR happens, generating 1 UVU photon
Volume Recombination cont.
Ionization only + Attachement + Mutual Neutralization + Volume Recombination
0.5 1.0 1.5 2.0 2.5 3.0 3.5 40000 45000 50000 55000 60000 65000 70000
Ionization only + Attachement + Mutual Neutralization + Volume Recombination
0.5 1.0 1.5 2.0 2.5 3.0 3.5 2.0×1011 4.0×1011 6.0×1011 8.0×1011 1.0×1012 1.2×1012
Attachment +Mutual Neutralization + Volume Recombination
0.5 1.0 1.5 2.0 2.5 3.0 3.5 1×1011 2×1011 3×1011 4×1011 Mutual Neutralization Volume Recombination Total
0.5 1.0 1.5 2.0 2.5 3.0 3.5 1×108 2×108 3×108 4×108 5×108 6×108 7×108
E field Vs X Ar2+ Vs X H2O- Vs X 𝜹 Vs X
VR:
𝐽A + 𝑓9 → γ
generates less γ than MN.
X[m] X[m]
E (V/m)
n+ [m-3] n- [m-3] [m-3 s-1]
Mutual Neutralization Volume Recombination Total
0.5 1.0 1.5 2.0 2.5 3.0 3.5 1×108 2×108 3×108 4×108 5×108 6×108 7×108
𝜹 rate Vs X Final E field Vs X +32%
Final solution (the red line) of E field has Eanode = 416 V/cm and Ecathode = 662 V/cm. This is a larger distortion comparing to the ProtoDUNE experimental measurements. Final solution (from our model) of photon production rate (the purple line) in the entire ProtoDUNE volume is: 6.3 X 1010 Hz
Use experimental observable to constrain the model parameters.
0.5 1.0 1.5 2.0 2.5 3.0 3.5 45000 50000 55000 60000 65000
- 17%
E (V/m)
X [m] X [m] [m-3 s-1]
Many parameters in our model are uncertain, next I will describe the impact of the size of the effect (mainly on the E field distortion and photon rate) by varying:
- Cosmic flux or other ionization source (Ar39)
- Lifetime: attachment rate to impurity and impurity concentration
- Ion mobility
- E field central value
Cosmic flux/Ar39
~ 10% seasonal variation of the cosmic flux. Ar39 beta decay is another source of the ionization charges (~1Bq/kg in natural Argon) – this add 0.5% of npair comparing to the cosmic at surface. Next I compare effect with standard cosmic flux to 10% higher cosmic flux.
Standard 10% higher cosmic flux
0.5 1.0 1.5 2.0 2.5 3.0 3.5 45000 50000 55000 60000 65000
Standard 10% higher cosmic flux
0.5 1.0 1.5 2.0 2.5 3.0 3.5 2×108 4×108 6×108 8×108
Photon production Vs X Standard 10% higher cosmic flux
0.5 1.0 1.5 2.0 2.5 3.0 3.5 2×1011 4×1011 6×1011 8×1011 1×1012
Hard to observe the E field change induced by the cosmic flux seasonal change. 10% higher cosmic flux -> 13% more photon rate.
E field Vs X Ar2+ Vs X Photon rate Vs X [m-3 s-1] X [m]
E (V/m)
n+ [m-3] X [m] X [m]
Purity / kA dependence:
Impurity concentration c[H2O] and e- attachment rate to impurity (kA) always couple together in our differential equation - , this term also proportional to 1/𝜐, where 𝜐 is the electron lifetime (a measureable quantity in the experiment) Intuitively, more impurities, more photons generated from the Mutual Neutralization. Prediction: effect negatively correlated with lifetime In this study, vary the product (c[H2O] * ka) from standard 6ms to 3ms, 2ms, 1.5ms
”purity” modifies the E field!
lifetime EA EC EC/E0 %
6ms
416 V/cm 662 V/cm [-17%,+32%]
3ms
437 V/cm 635 V/cm [-13%, +27%]
2ms
452 V/cm 613 V/cm [-10%,+23%]
1.5ms 463 V/cm
597 V/cm [-7%,+19%]
ka ka*2 ka*3 ka*4
0.5 1.0 1.5 2.0 2.5 3.0 3.5 45000 50000 55000 60000 65000
The data measurements of E field constrain the model to prefer shorter lifetime than 6ms.
E field Vs X
E (V/m) X [m]
decrease lifetime decrease lifetime Ar2+ density Vs X H2O- density Vs X
Decrease lifetime from 6ms to 2ms increase photon rate by 90%.
Comparing to SPE rate for different purity data samples are
- n-going.
0.5 1.0 1.5 2.0 2.5 3.0 3.5 2×1011 4×1011 6×1011 8×1011 1×1012 0.5 1.0 1.5 2.0 2.5 3.0 3.5 2×1010 4×1010 6×1010 8×1010 1×1011
ka ka*2 ka*3 ka*4
0.5 1.0 1.5 2.0 2.5 3.0 3.5 2.0×108 4.0×108 6.0×108 8.0×108 1.0×109 1.2×109 1.4×109
Photon production Vs X
Photon rate Vs X decrease lifetime
”purity” modifies photon rate!
6ms 3ms 2ms 1.5ms
[m-3 s-1] X [m]
Ion mobility dependence:
There could be a big uncertainty of the ion mobility. In the standard calculation we use 8x10-8 [m2 V-1 s-1] as Ar2+ mobility (this corresponds to 4x10-3 m/s drift velocity at 500V/cm Field). Intuitively, increase the mobility will decrease the density of the ions, which decrease the photon generation rate. Prediction: effect negatively correlated with ion mobility In this study, compare the effect with x2 of the standard mobility for both positive and negative ions.
Comparing to slower ion mobility
E field Vs X H2O- density Vs X
Twice of the ion mobility:
- Decrease E field
distortion from [-17%, +32%] to [-9%,+19%].
- Decrease the
photon rate by 21%.
Ar2+ density Vs X
Standard x2 ion mobility
0.5 1.0 1.5 2.0 2.5 3.0 3.5 45000 50000 55000 60000 65000
Standard x2 ion mobility
0.5 1.0 1.5 2.0 2.5 3.0 3.5 2×1011 4×1011 6×1011 8×1011 1×1012
Standard x2 ion mobility
0.5 1.0 1.5 2.0 2.5 3.0 3.5 1×1010 2×1010 3×1010 4×1010
Standard x2 ion mobility
0.5 1.0 1.5 2.0 2.5 3.0 3.5 1×108 2×108 3×108 4×108 5×108 6×108 7×108
Photon production Vs X
Photon production Vs X
E field dependence:
- higher E field, faster drift velocity, less ion densities, less photons.
- higher E field, less initial recombination, more Ar2+, more photons
Changing E field leads to two competing processes, that decides final photon generation rate. For simplicity, ignore the gauss law for this study. Vary E field from 500 V/cm to 200 V/cm with 50V/cm step.
As a function of E field
E field (V/cm)
Photon rate (entire volume) Vs E field
Photon rate at E0 = 250 V/cm is 60% higher of the rate at E0=500V/cm Comparing to the SPE measurements with different E field data samples are on-going.
Drift X [m]
E=500V/cm E=450V/cm E=400V/cm E=350V/cm E=300V/cm E=250V/cm E=200V/cm
0.5 1.0 1.5 2.0 2.5 3.0 3.5 2.0×108 4.0×108 6.0×108 8.0×108 1.0×109 1.2×109
Photon production Vs X
Photon generation rate Vs X
- 250
300 350 400 450 500 7.0×1010 8.0×1010 9.0×1010 1.0×1011 1.1×1011 1.2×1011
[m-3 s-1] [s-1]
Summary & Outlook
- We presented a model that describes the space charges (+ & -)
distributions and their impact to E field and photon generation. - done
- The model is robust – predict the trends that correlate with experimental
- bservables. - done
- The model contains many parameters that can be constrained by
protoDUNE data. – on-going
- This model can then be used to optimize the detector design to reduce
the single PE rate background and enable the LArTPC physics capability at low energy (link to my PONDD talk)
Backup
How big is the effect if we ignore the space charge distortion on the E field? – remove the Gauss Law from the differential equation set
Comparison of wi and wo Gauss law
Mostly change the positive ion distribution
Without Gauss Law With Gauss Law
0.5 1.0 1.5 2.0 2.5 3.0 3.5 2.0×1011 4.0×1011 6.0×1011 8.0×1011 1.0×1012 1.2×1012 1.4×1012
Positive ion Vs X
Without Gauss Law With Gauss Law
0.5 1.0 1.5 2.0 2.5 3.0 3.5 1×108 2×108 3×108 4×108 5×108 6×108 7×108
Photon production Vs X
13% lower photon rate if not considering Gauss Law