HL-LHC DA MD3312 FlatOptics MD2148 Joschua Dilly HL-LHC DA - - PowerPoint PPT Presentation

HL-LHC DA MD3312 — FlatOptics MD2148

Joschua Dilly

HL-LHC DA MD3312 — FlatOptics MD2148 2

Settings Delta Comparison MD2148 to MD3312 Why it’s the Tune Feedback Why it’s not the Separation Bumps Minor Conclusions Beam1 Data K-Modulation Results Between MD2148 to MD3312 MD3312 before and after corrections Beam2 Data Between MD2148 to MD3312 Conclusions Apendix Knob-Values

HL-LHC DA MD3312 — FlatOptics MD2148 3

Settings

HL-LHC DA MD3312 — FlatOptics MD2148 4

MD2148 MD3312

Beam 1 Beam 2 Beam 1 Beam 2 QX 0.2806 0.28 0.2805 0.2809 QY 0.3093 0.31 0.309 0.309 QXACD 0.2686 0.268 0.2685 0.2689 QYACD 0.3243 0.32 0.324 0.324 Optics

R2017aT65 A60 15C15 60A10mL300

Beam Process

SQUEEZE-6.5TeV-ATS-65cm-60 15cm-2017 V1 ATSFlat@526 [END] Orbit Bumps: 2018 flat orbitbump arc45

1.0 1.0

2018 flat q10r4 linked to orbitbump

1.0 1.0

Old Correction: 2018 global ats flat b1

1.0 1.0

2018 global ats flat b2

1.0 1.0

New Correction: 2018 global ats flat b1 for ip5 waist

0.0 0.8

HL-LHC DA MD3312 — FlatOptics MD2148 5

Delta Comparison MD2148 to MD3312

HL-LHC DA MD3312 — FlatOptics MD2148 6

Delta Comparison MD2148 to MD3312

In the following subsection all results represent the difference of the measurements between MD3312 and MD2148. Hence, there are additional ’∆’ symbols before the labels to indicate this difference.

HL-LHC DA MD3312 — FlatOptics MD2148 7

Subsection 1 Why it’s the Tune Feedback

HL-LHC DA MD3312 — FlatOptics MD2148 8

Delta Comparison MD2148 to MD3312

In the following slides, current measurements were used to calculate ∆K values, which were then in turn inserted into Madx to get their influence on the β-beating. The results are then compared to the measurements.

HL-LHC DA MD3312 — FlatOptics MD2148 9

Name 12-June [A] 30-October [A] ∆ [A] ∆K [10−5] kqtd.a12b1 14.61 15.66 1.05 1.08 kqtd.a23b1

• 100.58
• 94.73

5.85 6.04 kqtd.a34b1

• 107.97
• 102.11

5.86 6.05 kqtd.a45b1

• 23.72
• 22.68

1.04 1.07 kqtd.a56b1 32.29 33.34 1.05 1.08 kqtd.a67b1 106.75 112.62 5.87 6.06 kqtd.a78b1 119.84 125.68 5.84 6.03 kqtd.a81b1

• 20.86
• 19.81

1.05 1.08 kqtf.a12b1

• 19.99
• 14.76

5.23 5.40 kqtf.a23b1

• 28.37
• 19.72

8.65 8.93 kqtf.a34b1

• 22.52
• 13.85

8.67 8.95 kqtf.a45b1 18.29 23.5 5.21 5.38 kqtf.a56b1

• 36.03
• 30.81

5.22 5.39 kqtf.a67b1 69.76 78.43 8.67 8.95 kqtf.a78b1 58.62 67.29 8.67 8.95 kqtf.a81b1 16.34 21.54 5.2 5.37

Table: Beam1 Current measured during MD2148 and 3312 → big current differences in the ATS arcs due to tune feedback.

(Data thanks to Matteo Solfaroli Camillocci)

HL-LHC DA MD3312 — FlatOptics MD2148 10

5000 10000 15000 20000 25000 0.050 0.025 0.000 0.025 0.050

X/ X

kqtd.a12b1 kqtd.a23b1 kqtd.a34b1 kqtd.a45b1 kqtd.a56b1 kqtd.a67b1 kqtd.a78b1 kqtd.a81b1 kqtf.a12b1 kqtf.a23b1 kqtf.a34b1 kqtf.a45b1 kqtf.a56b1 kqtf.a67b1 kqtf.a78b1 kqtf.a81b1 all 5000 10000 15000 20000 25000 Longitudinal location [m] 0.01 0.00 0.01

Y/ Y

Figure: Beam 1 β-beating difference from current. → Strongest influencers clearly ATS-arcs.

HL-LHC DA MD3312 — FlatOptics MD2148 11

0.10 0.05 0.00 0.05 0.10

X/ X

from I from harmonic analysis 5000 10000 15000 20000 25000 0.10 0.05 0.00 0.05 0.10

Y/ Y

IP2 IP3 IP1 IP6 IP7 IP4 IP5 IP8

Figure: Beam 1 β-beating difference from current and harpy. → Differences are well explained by current measurements.

HL-LHC DA MD3312 — FlatOptics MD2148 12

Name 12-June [A] 30-October [A] ∆ [A] ∆K [10−5] kqtd.a12b2

• 7.55
• 6.96

0.59 0.61 kqtd.a23b2 139.05 147.61 8.56 8.84 kqtd.a34b2 142.59 151.15 8.56 8.83 kqtd.a45b2 35.24 35.82 0.58 0.60 kqtd.a56b2

• 29.09
• 28.51

0.58 0.60 kqtd.a67b2

• 70.84
• 62.28

8.56 8.83 kqtd.a78b2

• 94.61
• 86.06

8.55 8.82 kqtd.a81b2 33.2 33.79 0.59 0.61 kqtf.a12b2 8.62 8.8 0.18 0.19 kqtf.a23b2 63.83 81.48 17.65 18.22 kqtf.a34b2 58.78 76.43 17.65 18.22 kqtf.a45b2

• 34.11
• 33.92

0.19 0.20 kqtf.a56b2 28.91 29.1 0.19 0.20 kqtf.a67b2

• 34.73
• 17.08

17.65 18.22 kqtf.a78b2

• 8.71

8.93 17.64 18.21 kqtf.a81b2

• 31.31
• 31.12

0.19 0.20

Table: Beam2 Current measured during MD2148 and 3312 → only small current differences in the ATS arcs.

(Data thanks to Matteo Solfaroli Camillocci)

HL-LHC DA MD3312 — FlatOptics MD2148 13

5000 10000 15000 20000 25000 0.015 0.010 0.005 0.000 0.005

X/ X

kqtd.a12b2 kqtd.a23b2 kqtd.a34b2 kqtd.a45b2 kqtd.a56b2 kqtd.a67b2 kqtd.a78b2 kqtd.a81b2 kqtf.a12b2 kqtf.a23b2 kqtf.a34b2 kqtf.a45b2 kqtf.a56b2 kqtf.a67b2 kqtf.a78b2 kqtf.a81b2 all 5000 10000 15000 20000 25000 Longitudinal location [m] 0.005 0.000 0.005 0.010

Y/ Y

Figure: Beam 2 β-beating difference from current. → The high values in the non-ATS arcs have little influence.

HL-LHC DA MD3312 — FlatOptics MD2148 14

0.10 0.05 0.00 0.05 0.10

X/ X

from I from harmonic analysis 5000 10000 15000 20000 25000 0.10 0.05 0.00 0.05 0.10

Y/ Y

IP2 IP3 IP1 IP6 IP7 IP4 IP5 IP8

Figure: Beam 2 β-beating difference from current and harpy. → Differences might be due to noisy measurements.

HL-LHC DA MD3312 — FlatOptics MD2148 15

Subsection 2 Why it’s not the Separation Bumps

HL-LHC DA MD3312 — FlatOptics MD2148 16

Delta Comparison MD2148 to MD3312

In the following slides, as model, the difference between models with and without separation bumps in IP1 and IP5 are used, as this was the only ”manual” settings difference discovered.

HL-LHC DA MD3312 — FlatOptics MD2148 17

0.0 0.2 0.4 0.6 X [mm] Model Measurement 5000 10000 15000 20000 25000 Longitudinal location [m] 0.0 0.2 0.4 0.6 Y [mm] IP2 IP3 IP1 IP6 IP7 IP4 IP5 IP8

Figure: Beam 1 Orbit difference MD3312 and MD2148.

→ Model and Measurement are in agreement

HL-LHC DA MD3312 — FlatOptics MD2148 18

0.10 0.05 0.00 0.05 0.10

X/ X

Model Measurement 5000 10000 15000 20000 25000 Longitudinal location [m] 0.10 0.05 0.00 0.05 0.10

Y/ Y

IP2 IP3 IP1 IP6 IP7 IP4 IP5 IP8

Figure: Beam 1 β-beating difference MD3312 and MD2148.

→ ≈ 5% unexplained β-beating in X-plane measurement.

HL-LHC DA MD3312 — FlatOptics MD2148 19

2 1 1 X [mm] Model Measurement 5000 10000 15000 20000 25000 Longitudinal location [m] 2 1 1 Y [mm] IP2 IP3 IP1 IP6 IP7 IP4 IP5 IP8

Figure: Beam 2 Orbit difference MD3312 and MD2148.

→ Model and Measurement are in agreement

HL-LHC DA MD3312 — FlatOptics MD2148 20

0.10 0.05 0.00 0.05 0.10

X/ X

Model Measurement 5000 10000 15000 20000 25000 Longitudinal location [m] 0.10 0.05 0.00 0.05 0.10

Y/ Y

IP2 IP3 IP1 IP6 IP7 IP4 IP5 IP8

Figure: Beam 2 β-beating difference MD3312 and MD2148.

→ Differences in X-plane not as clear as for Beam1 (maybe unexplained)

HL-LHC DA MD3312 — FlatOptics MD2148 21

Subsection 3 Minor Conclusions

HL-LHC DA MD3312 — FlatOptics MD2148 22

Conclusions

• Current differences between the MDs explain Beam 1 β-beating

very well.

• Orbit bumps have only minor influence.
• Beam 2 β-beating not completely explained.

HL-LHC DA MD3312 — FlatOptics MD2148 23

Beam1 Data

HL-LHC DA MD3312 — FlatOptics MD2148 24

Subsection 1 K-Modulation Results

HL-LHC DA MD3312 — FlatOptics MD2148 25

IP1 IP5 X Y X Y MD2148

Final Result

β∗[m] —* 0.166 0.180 0.596 Waist [m] —* 0.049

• 0.067

0.067 βWaist [m] —* 0.150 0.151 0.588 MD3312

Before Corr.

β∗[m] — — 0.241 0.699 Waist [m] — —

• 0.116

0.221 βWaist [m] — — 0.151 0.621 MD3312

After Corr.

β∗[m] — — 0.169 0.640 Waist [m] — —

• 0.052

0.040 βWaist [m] — — 0.151 0.637 * bad k-modulation measurement

HL-LHC DA MD3312 — FlatOptics MD2148 26

Subsection 2 Between MD2148 to MD3312

HL-LHC DA MD3312 — FlatOptics MD2148 27

2 2 4 x [mm] mo_MD2148 mo_MD3312 me_MD2148 me_MD3312 5000 10000 15000 20000 25000 Longitudinal location [m] 2 1 1 2 y [mm] IP2 IP3 IP1 IP6 IP7 IP4 IP5 IP8

Figure: Orbit comparison MD2148 and MD3312

HL-LHC DA MD3312 — FlatOptics MD2148 28

0.2 0.1 0.0 0.1 0.2

x/ x

MD2148 MD3312 5000 10000 15000 20000 25000 Longitudinal location [m] 0.15 0.10 0.05 0.00 0.05 0.10 0.15

y/ y

IP2 IP3 IP1 IP6 IP7 IP4 IP5 IP8

Figure: Beta-Beating comparison MD2148 and MD3312

HL-LHC DA MD3312 — FlatOptics MD2148 29

0.01 0.00 0.01

x

[2 ] MD2148 MD3312 5000 10000 15000 20000 25000 Longitudinal location [m] 0.015 0.010 0.005 0.000 0.005 0.010 0.015

y

[2 ] IP2 IP3 IP1 IP6 IP7 IP4 IP5 IP8

Figure: Phase comparison MD2148 and MD3312

HL-LHC DA MD3312 — FlatOptics MD2148 30

0.05 0.00 0.05 0.10 0.15 |f1001| MD2148 MD3312 5000 10000 15000 20000 25000 Longitudinal location [m] 0.05 0.00 0.05 0.10 |f1010| IP2 IP3 IP1 IP6 IP7 IP4 IP5 IP8

Figure: Coupling Amp. comparison MD2148 and MD3312

HL-LHC DA MD3312 — FlatOptics MD2148 31

Subsection 3 MD3312 before and after corrections

HL-LHC DA MD3312 — FlatOptics MD2148 32

2 1 1 2 x [mm] mo_Before_Correction mo_After_Correction me_Before_Correction me_After_Correction 5000 10000 15000 20000 25000 Longitudinal location [m] 3 2 1 1 y [mm] IP2 IP3 IP1 IP6 IP7 IP4 IP5 IP8

Figure: Orbit comparison MD3312 before and after corrections.

HL-LHC DA MD3312 — FlatOptics MD2148 33

0.1 0.0 0.1 0.2

x/ x

Before_Correction After_Correction 5000 10000 15000 20000 25000 Longitudinal location [m] 0.1 0.0 0.1

y/ y

IP2 IP3 IP1 IP6 IP7 IP4 IP5 IP8

Figure: Beta-Beating comparison MD3312 before and after corrections.

HL-LHC DA MD3312 — FlatOptics MD2148 34

0.02 0.00 0.02

x

[2 ] Before_Correction After_Correction 5000 10000 15000 20000 25000 Longitudinal location [m] 0.01 0.00 0.01

y

[2 ] IP2 IP3 IP1 IP6 IP7 IP4 IP5 IP8

Figure: Phase comparison MD3312 before and after corrections.

HL-LHC DA MD3312 — FlatOptics MD2148 35

0.025 0.000 0.025 0.050 0.075 0.100 |f1001| Before_Correction After_Correction 5000 10000 15000 20000 25000 Longitudinal location [m] 0.025 0.000 0.025 0.050 0.075 |f1010| IP2 IP3 IP1 IP6 IP7 IP4 IP5 IP8

Figure: Coupling Amp. comparison MD3312 before and after corrections.

HL-LHC DA MD3312 — FlatOptics MD2148 36

Beam2 Data

HL-LHC DA MD3312 — FlatOptics MD2148 37

Subsection 1 Between MD2148 to MD3312

HL-LHC DA MD3312 — FlatOptics MD2148 38

2 2 4 x [mm] mo_MD2148 mo_MD3312 me_MD2148 me_MD3312 5000 10000 15000 20000 25000 Longitudinal location [m] 2 1 1 2 y [mm] IP2 IP3 IP1 IP6 IP7 IP4 IP5 IP8

Figure: Orbit comparison MD2148 and MD3312

HL-LHC DA MD3312 — FlatOptics MD2148 39

0.2 0.1 0.0 0.1 0.2

x/ x

MD2148 MD3312 5000 10000 15000 20000 25000 Longitudinal location [m] 0.15 0.10 0.05 0.00 0.05 0.10 0.15

y/ y

IP2 IP3 IP1 IP6 IP7 IP4 IP5 IP8

Figure: Beta-Beating comparison MD2148 and MD3312

HL-LHC DA MD3312 — FlatOptics MD2148 40

0.01 0.00 0.01

x

[2 ] MD2148 MD3312 5000 10000 15000 20000 25000 Longitudinal location [m] 0.015 0.010 0.005 0.000 0.005 0.010 0.015

y

[2 ] IP2 IP3 IP1 IP6 IP7 IP4 IP5 IP8

Figure: Phase comparison MD2148 and MD3312

HL-LHC DA MD3312 — FlatOptics MD2148 41

0.05 0.00 0.05 0.10 0.15 |f1001| MD2148 MD3312 5000 10000 15000 20000 25000 Longitudinal location [m] 0.05 0.00 0.05 0.10 |f1010| IP2 IP3 IP1 IP6 IP7 IP4 IP5 IP8

Figure: Coupling Amp. comparison MD2148 and MD3312

HL-LHC DA MD3312 — FlatOptics MD2148 42

Conclusions

HL-LHC DA MD3312 — FlatOptics MD2148 43

Conclusions

• ”Corrections” lower targeted β∗ but not as far as hoped
• ... while at the same time inducing max. β-beating of 21%

HL-LHC DA MD3312 — FlatOptics MD2148 44

Apendix

HL-LHC DA MD3312 — FlatOptics MD2148 45

Subsection 1 Knob-Values

HL-LHC DA MD3312 — FlatOptics MD2148 46

2018 flat orbitbump arc45

acbh20.r4b1 = 1.85 · 10−05 acbh28.r4b1 = 1.08 · 10−05 acbh16.r4b1 = −3.38 · 10−06 acbh24.r4b1 = 1.18 · 10−05

2018 flat q10r4 linked to orbitbump

kq10.r4b1 = 7.4158270790E-03;

HL-LHC DA MD3312 — FlatOptics MD2148 47

2018 global ats flat b1

kqtl11.r6b1 = 2.44 · 10−05 kqt12.l1b1 = −9.61 · 10−04 kq10.l4b1 = −6.38 · 10−03 kq7.r8b1 = −7.35 · 10−03 kq5.l1b1 = −2.16 · 10−03 kq5.r2b1 = −4.11 · 10−03 kq10.r6b1 = 7.00 · 10−03 kq4.r5b1 = −2.59 · 10−03 kq9.r2b1 = −5.53 · 10−03 kqt12.r2b1 = −3.50 · 10−04 kq8.r4b1 = 8.55 · 10−03 kq4.r6b1 = 5.66 · 10−03 kq8.l4b1 = −5.27 · 10−03 kqt12.r3b1 = 4.99 · 10−03 kqtl11.r7b1 = −9.84 · 10−05 kq9.r1b1 = 6.60 · 10−03 kq10.r5b1 = −6.77 · 10−03 kqtl11.l5b1 = 1.06 · 10−03 kqt12.l2b1 = −1.06 · 10−03 kqtl7.l3b1 = −1.99 · 10−03 kq4.l5b1 = 2.60 · 10−03 kq8.r5b1 = −7.13 · 10−03 kqtd.a45b1 = 2.54 · 10−04 kqt13.l8b1 = 8.33 · 10−04 kqt13.r1b1 = −1.82 · 10−04 kq10.r4b1 = 7.42 · 10−03 kq6.l8b1 = −5.58 · 10−03 kq8.l5b1 = 7.79 · 10−03 kq6.r1b1 = −1.84 · 10−03 kqtl8.r3b1 = 2.50 · 10−03 kqtd.a12b1 = −1.70 · 10−04 kq10.l5b1 = 7.06 · 10−03 kqtl11.r4b1 = −2.71 · 10−03 kq9.l1b1 = −6.73 · 10−03 kq10.l2b1 = −6.46 · 10−03 kqt12.l3b1 = 2.84 · 10−03 kq8.l2b1 = −5.48 · 10−03 kqtl11.l4b1 = 7.95 · 10−04 kqtl11.l7b1 = 2.24 · 10−03 kq4.l1b1 = 2.57 · 10−03 kqtf.a12b1 = −1.67 · 10−04 kq4.r8b1 = 3.05 · 10−03 kq8.r2b1 = 6.33 · 10−03 kq4.r2b1 = 3.10 · 10−03 kq5.l4b1 = 4.16 · 10−03 kqtl11.l8b1 = −1.36 · 10−04 kqt12.l4b1 = −2.83 · 10−03 kq8.l1b1 = 7.79 · 10−03 kqt13.r3b1 = −4.56 · 10−03 kqtd.a78b1 = −1.33 · 10−03 kq8.r1b1 = −7.13 · 10−03 kq9.r4b1 = −6.32 · 10−03 kq9.l4b1 = 6.94 · 10−03 kqtl11.l2b1 = 7.98 · 10−04 kq4.l2b1 = −3.11 · 10−03 kq8.r8b1 = 7.64 · 10−03 kqtd.a56b1 = −3.65 · 10−04 kq4.l8b1 = −3.05 · 10−03 kq7.r5b1 = 7.10 · 10−03 kqtl9.r7b1 = 3.78 · 10−03 kqt12.r1b1 = −3.71 · 10−03 kqt12.r4b1 = −4.20 · 10−04 kqt12.r7b1 = 1.93 · 10−03 kqtf.a78b1 = 7.03 · 10−04 kq7.l2b1 = 7.59 · 10−03 kqtl9.l7b1 = 2.76 · 10−04 kq7.l5b1 = −7.31 · 10−03 kq6.r3b1 = −2.49 · 10−03 kq7.l8b1 = 8.06 · 10−03 kqtd.a81b1 = 2.22 · 10−04 kqtf.a56b1 = −3.44 · 10−04 kqt13.l3b1 = −6.35 · 10−04 kqt13.l6b1 = −1.67 · 10−03 kq6.l3b1 = 2.65 · 10−03 kqtl11.r2b1 = −1.10 · 10−03 kqtl11.r5b1 = −3.98 · 10−05 kqtl7.r3b1 = 9.09 · 10−04 kqtf.a34b1 = −1.95 · 10−04 kq10.l6b1 = −7.94 · 10−03 kq5.r1b1 = 2.06 · 10−03 kqtl11.r8b1 = 9.06 · 10−04 kq5.r4b1 = −4.01 · 10−03 kq6.r5b1 = −1.85 · 10−03 kq9.l6b1 = 6.71 · 10−03 kqtl9.l3b1 = −4.71 · 10−03 kq7.r2b1 = −6.22 · 10−03 kqt12.l7b1 = 8.27 · 10−04 kqt12.r8b1 = −3.57 · 10−03 kqtl10.r3b1 = 2.85 · 10−03 kqt13.l4b1 = 3.06 · 10−03 kqt13.r5b1 = −1.81 · 10−04 kq5.r8b1 = −2.70 · 10−03 kqtl8.r7b1 = 9.58 · 10−04 kq7.l1b1 = −7.35 · 10−03 kq9.r8b1 = −7.39 · 10−03 kq6.l4b1 = −5.14 · 10−03 kqtd.a67b1 = −1.19 · 10−03 kqt13.r6b1 = 4.66 · 10−03 kqt12.l8b1 = 2.41 · 10−03 kq9.r6b1 = −6.66 · 10−03 kq6.l2b1 = −5.10 · 10−03 kq6.l5b1 = 1.74 · 10−03 kqt13.l5b1 = 1.56 · 10−03 kqtl10.l3b1 = 9.16 · 10−04 kq10.r1b1 = −6.76 · 10−03 kqtd.a34b1 = 1.18 · 10−03 kqtd.a23b1 = 1.10 · 10−03 kqt13.l2b1 = 3.10 · 10−03 kq8.l8b1 = −6.59 · 10−03 kqtl8.l7b1 = −6.24 · 10−04 kqtf.a81b1 = 2.34 · 10−04 kqtl11.r1b1 = −4.49 · 10−05 kq5.l6b1 = 7.17 · 10−03 kqt12.l6b1 = −2.94 · 10−03 kqtl11.l1b1 = 1.05 · 10−03 kq6.r4b1 = 4.69 · 10−03 kqt13.r7b1 = 1.11 · 10−03 kq6.r7b1 = −3.12 · 10−03 kq4.r1b1 = −2.57 · 10−03 kqt13.r4b1 = 4.04 · 10−03 kq6.r2b1 = 4.11 · 10−03 kqtl11.r3b1 = −3.63 · 10−03 kq8.l6b1 = −5.40 · 10−03 kq6.r8b1 = 4.55 · 10−03 kqt13.l1b1 = 1.56 · 10−03 kqt13.r2b1 = −1.86 · 10−03 kqt12.r5b1 = −3.71 · 10−03 kq5.r5b1 = 2.05 · 10−03 kqt13.r8b1 = 3.69 · 10−03 kq10.r2b1 = 7.24 · 10−03 kqtl7.l7b1 = 1.59 · 10−03 kqtl7.r7b1 = 4.99 · 10−03 kqtl10.r7b1 = −8.60 · 10−04 kqt12.r6b1 = 4.27 · 10−03 kq10.r8b1 = 7.33 · 10−03 kq6.l7b1 = 3.25 · 10−03 kq10.l8b1 = −5.76 · 10−03 kq5.r6b1 = −6.55 · 10−03 kq9.r5b1 = 6.59 · 10−03 kqt12.l5b1 = −9.61 · 10−04 kq6.l1b1 = 1.74 · 10−03 kq10.l1b1 = 7.06 · 10−03 kq7.l4b1 = 7.23 · 10−03 kqtl8.l3b1 = 1.27 · 10−04 kqtl11.l6b1 = −1.44 · 10−03 kq5.l8b1 = 3.76 · 10−03 kq5.l5b1 = −2.14 · 10−03 kq8.r6b1 = 7.20 · 10−03 kqtf.a67b1 = 8.26 · 10−04 kq7.r1b1 = 7.11 · 10−03 kqtl9.r3b1 = −7.13 · 10−05 kqtl11.l3b1 = −3.39 · 10−04 kqtf.a45b1 = 2.56 · 10−04 kq7.r4b1 = −5.01 · 10−03 kq9.l8b1 = 6.65 · 10−03 kqtl10.l7b1 = 4.48 · 10−03 kq9.l2b1 = 6.88 · 10−03 kqtf.a23b1 = −2.60 · 10−04 kq9.l5b1 = −6.73 · 10−03

HL-LHC DA MD3312 — FlatOptics MD2148 48

2018 global ats flat b2

kqtl9.r3b2 = −3.98 · 10−03 kq6.l2b2 = 4.43 · 10−03 kq9.r6b2 = 7.08 · 10−03 kqt12.r7b2 = −2.03 · 10−03 kqtd.a34b2 = −1.57 · 10−03 kq5.l5b2 = 1.75 · 10−03 kq8.l8b2 = 6.73 · 10−03 kqt13.l2b2 = 1.97 · 10−03 kqtd.a81b2 = −3.59 · 10−04 kq7.r1b2 = −7.03 · 10−03 kq6.r3b2 = 2.68 · 10−03 kqt12.l6b2 = 4.78 · 10−03 kqtf.a45b2 = −3.83 · 10−04 kq5.l6b2 = −6.84 · 10−03 kq6.r4b2 = −6.33 · 10−03 kq6.l3b2 = −2.45 · 10−03 kq9.l5b2 = 6.68 · 10−03 kqt13.l3b2 = −5.07 · 10−03 kqt13.r4b2 = −3.64 · 10−03 kq5.r5b2 = −1.91 · 10−03 kqt12.r8b2 = −2.01 · 10−03 kqt13.l1b2 = −6.15 · 10−04 kqt12.r5b2 = −1.77 · 10−03 kqt13.l4b2 = −2.75 · 10−03 kq9.l6b2 = −6.18 · 10−03 kqtl7.r7b2 = 2.44 · 10−05 kqtl7.l7b2 = 4.20 · 10−03 kq9.r8b2 = 7.02 · 10−03 kqt13.r3b2 = −6.33 · 10−04 kq6.l4b2 = 5.77 · 10−03 kq9.r5b2 = −6.96 · 10−03 kqt13.r6b2 = −1.71 · 10−03 kqt12.l5b2 = −1.40 · 10−03 kq7.r2b2 = 7.17 · 10−03 kq6.l1b2 = −1.63 · 10−03 kqt12.l8b2 = −1.18 · 10−03 kqtl8.l3b2 = 2.18 · 10−03 kq5.l8b2 = −3.04 · 10−03 kqtl11.l6b2 = 3.06 · 10−03 kqtd.a45b2 = −3.82 · 10−04 kq6.l5b2 = −1.66 · 10−03 kq5.l2b2 = −3.63 · 10−03 kq8.r6b2 = −5.32 · 10−03 kqt13.l5b2 = −6.14 · 10−04 kqtd.a23b2 = −1.53 · 10−03 kqtl8.l7b2 = 1.41 · 10−03 kq10.l5b2 = −6.78 · 10−03 kqtl11.r1b2 = 1.15 · 10−04 kqtf.a81b2 = −3.52 · 10−04 kq7.r4b2 = 5.08 · 10−03 kqt12.l3b2 = 9.19 · 10−04 kqtl11.l1b2 = −2.29 · 10−04 kq9.l8b2 = −6.34 · 10−03 kqtl11.l7b2 = 1.26 · 10−04 kq4.r1b2 = 2.44 · 10−03 kq9.l2b2 = −7.14 · 10−03 kq6.r2b2 = −4.26 · 10−03 kqtl9.l3b2 = −3.85 · 10−06 kq8.l6b2 = 8.50 · 10−03 kq6.r8b2 = −5.36 · 10−03 kqt13.r5b2 = 4.54 · 10−03 kq6.r5b2 = 1.66 · 10−03 kqt13.r2b2 = 7.73 · 10−04 kq10.r8b2 = −6.28 · 10−03 kqt13.r8b2 = 3.91 · 10−03 kq7.l4b2 = −5.07 · 10−03 kqt12.r6b2 = 4.75 · 10−03 kq7.l1b2 = 7.13 · 10−03 kq10.r2b2 = −6.03 · 10−03 kqtl8.r7b2 = 1.28 · 10−03 kq5.r6b2 = 6.44 · 10−03 kq10.r5b2 = 7.22 · 10−03 kqtd.a67b2 = 7.92 · 10−04 kqtl11.r7b2 = 1.16 · 10−03 kq10.l8b2 = 7.28 · 10−03 kqt12.r3b2 = 2.80 · 10−03 kqtl11.l3b2 = −3.41 · 10−03 kq10.r4b2 = −5.94 · 10−03 kqt13.l8b2 = 1.31 · 10−03 kq6.l8b2 = 5.21 · 10−03 kq4.l2b2 = 3.49 · 10−03 kqtl9.l7b2 = 3.89 · 10−03 kqtf.a67b2 = −3.89 · 10−04 kq10.l2b2 = 7.26 · 10−03 kqtd.a12b2 = 9.12 · 10−05 kq7.l5b2 = 7.12 · 10−03 kqtl11.r4b2 = 8.52 · 10−04 kqtl10.l7b2 = 7.06 · 10−04 kqtl7.r3b2 = −2.80 · 10−03 kqtl11.l4b2 = −2.27 · 10−04 kq8.l2b2 = 7.31 · 10−03 kq5.r1b2 = −1.92 · 10−03 kqtl11.r5b2 = 1.18 · 10−04 kqtf.a23b2 = 7.01 · 10−04 kqt12.r1b2 = −1.77 · 10−03 kqtl11.r3b2 = 1.11 · 10−03 kqtl11.r6b2 = 1.30 · 10−03 kq10.l4b2 = 7.15 · 10−03 kq5.r2b2 = 4.32 · 10−03 kq7.r8b2 = 6.86 · 10−03 kqt12.r2b2 = −1.03 · 10−03 kq10.r6b2 = −7.53 · 10−03 kq9.r2b2 = 6.44 · 10−03 kq4.l1b2 = −2.47 · 10−03 kq8.r4b2 = −7.54 · 10−03 kqt13.l7b2 = −4.19 · 10−04 kq6.l7b2 = −2.97 · 10−03 kqtl10.r7b2 = 4.74 · 10−03 kq8.r1b2 = 7.73 · 10−03 kq8.l4b2 = 8.34 · 10−03 kq8.l1b2 = −7.56 · 10−03 kqt12.l2b2 = −2.70 · 10−03 kq10.l1b2 = −6.81 · 10−03 kq7.r5b2 = −7.08 · 10−03 kqtl9.r7b2 = −5.01 · 10−04 kqtf.a78b2 = −1.01 · 10−04 kqtl8.r3b2 = −1.47 · 10−04 kqtl10.l3b2 = 2.14 · 10−03 kq7.l2b2 = −7.92 · 10−03 kq10.r1b2 = 7.22 · 10−03 kqt12.r4b2 = 1.76 · 10−03 kq7.l8b2 = −5.89 · 10−03 kq9.l1b2 = 6.66 · 10−03 kqtf.a56b2 = 3.14 · 10−04 kqt13.l6b2 = −1.13 · 10−03 kq6.r1b2 = 1.66 · 10−03 kq8.l5b2 = −7.56 · 10−03 kq5.r4b2 = 5.35 · 10−03 kqtf.a34b2 = 6.45 · 10−04 kqt13.r7b2 = 1.84 · 10−03 kqtl11.r2b2 = 5.77 · 10−04 kqt13.r1b2 = 4.53 · 10−03 kqtl11.r8b2 = 2.26 · 10−04 kq10.l6b2 = 7.04 · 10−03 kq6.r7b2 = 3.32 · 10−03 kqtf.a12b2 = 9.00 · 10−05 kqt12.l1b2 = −1.40 · 10−03 kqtl10.r3b2 = 8.46 · 10−04 kq4.r8b2 = −3.37 · 10−03 kq8.r2b2 = −5.15 · 10−03 kq5.l1b2 = 1.76 · 10−03 kq4.r2b2 = −3.48 · 10−03 kq9.r4b2 = 6.06 · 10−03 kqt12.l7b2 = 4.26 · 10−03 kq5.l4b2 = −4.15 · 10−03 kqt12.l4b2 = 2.09 · 10−03 kq4.r5b2 = 2.45 · 10−03 kqtl11.l8b2 = −1.14 · 10−03 kqtd.a78b2 = 1.05 · 10−03 kq9.r1b2 = −6.95 · 10−03 kqtl11.l5b2 = −2.31 · 10−04 kq9.l4b2 = −5.04 · 10−03 kq8.r5b2 = 7.73 · 10−03 kqtd.a56b2 = 3.29 · 10−04 kqtl7.l3b2 = 7.67 · 10−04 kqtl11.l2b2 = 9.98 · 10−04 kq4.l8b2 = 3.38 · 10−03 kq4.l5b2 = −2.44 · 10−03 kq8.r8b2 = −6.86 · 10−03

HL-LHC DA MD3312 — FlatOptics MD2148 49