Simultaneous Four-Hall Operation for 12 GeV CEBAF Reza Kazimi November 2012.

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Presentation transcript:

Simultaneous Four-Hall Operation for 12 GeV CEBAF Reza Kazimi November 2012

2 November 30, 2012 Reza KazimiFour Hall Operation D+3 What is being proposed? Capability Planned Design (D+2)New Design (D+3) Maximum number of halls receiving beam simultaneously 3 Halls4 Halls The existing extraction design allows the simultaneous operation of Hall D, plus two other halls (D+2). We propose a design that allows the simultaneous operation of all four halls (D+3). How? Use a different frequency for the horizontal 5 th pass separator (750 MHz instead of 500 MHz). No changes to lower passes (Hall D wants only 5 th pass beam). Cut the beam bunch repetition rate for the halls taking 5 th pass beam in half (to 250 MHz). Total current to each hall can remain the same.

3 November 30, 2012 Reza KazimiFour Hall Operation D+3 RF Separator Location RF separators direct the beam to a hall or recirculate it for additional acceleration.

RF Separation Basics YA Magnet (septa) YA Magnet (septa) YB Magnet Beam To Halls Beam To Halls Recirculated Beam Recirculated Beam RF Separator RF separator creates small separation angle (~300 µradians) YA & YB magnets increase separation

B B C C B B A A A A C C B B A A C C B B A A C C B B A A C C B B A A C C B B A A C C C C B B A A C C B B A A C C B B A A C C B B A A C C B B A A C C C C B B A A C C B B A A C C B B A A C C B B A A C C B B A A C C C C B B A A C C B B A A C C B B A A C C B B A A C C B B A A C C C C B B A A C C B B A A C C B B A A C C B B A A C C B B A A C C C C B B A A C C B B A A C C B B A A C C B B A A C C B B A A C C C C B B A A C C B B A A C C B B A A C C B B A A C C B B A A C C C C B B A A C C B B A A C C B B A A C C B B A A C C B B A A C C C C B B A A C C B B A A C C B B A A C C B B A A C C B B A A C C B B A A C C B B A A C C B B A A C C C C B B A A C C B B A A C C C C B B A A C C B B A A C C B B A A C C B B A A C C B B A A C C Accelerator Frequency 1500 MHz Accelerator Frequency 1500 MHz RF Separator Cavity 500 MHz RF Separator Cavity 500 MHz Beam to Halls Recirculated Beams Recirculated Beams Separator frequency is 1/3 of the fundamental frequency Beam Turn on RF separator RF Separation – Existing (500 MHz) B B B B B B B B B B B B B B A A A A A A A A A A A A A A C C C C C C C C C C C C C C Hall Lasers Hall A: 500 MHz Hall Lasers Hall A: 500 MHz Hall C: 500 MHz Hall B: 500 MHz

A A B B A A C C C C B B A A C C B B A A C C B B A A C C B B A A C C B B A A C C B B Accelerator Frequency 1500 MHz Accelerator Frequency 1500 MHz 5 th Pass RF Separator Cavity 500 MHz 5 th Pass RF Separator Cavity 500 MHz Beam to Halls Beam to Hall D Beam D+2 (500 MHz) Hall D Separation D D D D D D D D D D D D D D Hall D replaces Hall A (limited to 3-hall operation) Hall D replaces Hall A (limited to 3-hall operation)

B B C C B B A A A A 5 th Pass RF Separator Cavity 750 MHz 5 th Pass RF Separator Cavity 750 MHz Beam to Halls Hall D Beam Hall D Beam Separator frequency is 1/2 of the fundamental frequency Beam Turn on RF separator RF Separation – Proposed (750 MHz) C C B B A A C C B B A A C C B B A A C C B B A A C C B B A A C C C C B B A A C C B B A A C C C C B B A A C C B B A A C C B B A A C C B B A A C C B B A A C C C C B B A A C C B B A A C C B B A A C C B B A A C C B B A A C C C C B B A A C C B B A A C C B B A A C C B B A A C C B B A A C C C C B B A A C C B B A A C C B B A A C C B B A A C C B B A A C C C C B B A A C C B B A A C C B B A A C C B B A A C C B B A A C C C C B B A A C C B B A A C C B B A A C C B B A A C C B B A A C C C C B B A A C C B B A A C C B B A A C C B B A A C C B B A A C C C C B B A A C C B B A A C C B B A A C C B B A A C C B B A A C C C C B B A A C C B B A A C C B B A A C C B B A A C C B B A A C C C C B B A A C C B B A A C C B B A A 500 MHz 750 MHz Proposed Frequency Proposed Frequency B B C C B B A A A A C C B B A A C C B B A A C C C C B B A A C C B B A A C C B B A A D D D A/B/C separator is located downstream Empty Buckets – Cutting the laser pulse rate for each hall in half (from 500 MHz to 250 MHz) leaves “empty buckets”, which are directed to Hall D Hall Lasers Hall A: 250 MHz Hall B: 250 MHz Hall C: 250 MHz Hall Lasers Hall A: 250 MHz Hall B: 250 MHz Hall C: 250 MHz New Hall D laser fills empty buckets at 250 MHz Hall D: 250 MHz Every other “bucket” goes to Hall D (existing hall lasers run at 500 MHz) Accelerator Frequency 1500 MHz Accelerator Frequency 1500 MHz Four-Hall Operation! (D+3) Four-Hall Operation! (D+3)

November 30, 2012 Reza KazimiFour Hall Operation D th Pass RF Separation Hardware Horizontal 5 th Pass Separator (kicks out Hall D) Horizontal 5 th Pass Separator (kicks out Hall D) D+2: 500 MHz D+3: 750 MHz

9 November 30, 2012 Reza KazimiFour Hall Operation D+3 Comparing D+2 and D+3 Planned (D+2)Proposed (D+3) Maximum number of halls receiving beam 3 halls4 halls 5 th pass (Hall D on)500 MHz250 MHz 5 th pass (Hall D off)500 MHz lower passes500 MHz The D+3 Tradeoff: On 5 th pass, all halls must run at 250 MHz (half the rep rate), unless Hall D is off. When Hall D is on, at least one hall must configured for the 5 th pass.

10 November 30, 2012 Reza KazimiFour Hall Operation D+3 Charge/Bunch at 5 th Pass MHz 180 µ A, max for 6 GeV 0.36 pC/bunch 0.72 pC/bunch 85 µ A, max for 12 GeV 0.17 pC/bunch 0.34 pC/bunch Combined current to Halls A and C will be limited to 85 µ A because of 1 mW total power limit. Charge/bunch for 85 µ A at 250 MHz is lower than the charge/bunch for 180 µ A at 500 MHz. The higher charger/bunch has already been demonstrated during 6 GeV operations (Qweak experiment). The impact of doubling the charge/bunch on experiments limited by accidental rates should be evaluated.

11 November 30, 2012 Reza KazimiFour Hall Operation D+3 Separator Cavity Design 500 MHz cavity 750 MHz cavity Beam Note: vertical cross sections shown 60 cm 40 cm Existing 500 MHz design is shortened for 750 MHz

12 November 30, 2012 Reza KazimiFour Hall Operation D+3 5 th Pass Separators Frequency500 MHz750 MHz Beam energy11 GeV Total separation angle 300  rad Number of Cavities44 Total RF power5.6 kW8 kW RF power per cavity1.4 kW2 kW Length of each cavity60 cm40 cm

13 November 30, 2012 Reza KazimiFour Hall Operation D+3 Generating 250 MHz Beams 250 MHz beams are required for D+3 to work. 500 MHz beams can also be used depending on the configuration. Some experiments like to run at lower repetition rates. A new CEBAF injector low-level laser drive system has been proposed by John Hansknecht that uses elector-optic modulators (a telecom standard) to produce 250 MHz beams.  Only affects front-end laser seed drivers. No changes to laser table components.  Gives any hall a “pushbutton” selectable running frequency of 500 MHz or lower divisions of 250, 125, 62.5, or MHz, without affecting other halls.  Replaces the beat frequency modulator—an additional advantage.  Will permit introduction of a 4 th laser for Hall D.  ~$100K

November 30, 2012 Reza KazimiFour Hall Operation D+3 14 RF Separator Evolution & Cost 6 GeV Configuration D + 1 D + 2 D + 3 Key New Relocated 750 MHz Cavities 500 MHz Cavities D+2 & D MHz Cavities D+2 & D+3 Total Cost D+1$ 507K Total Cost D+1$ 507K D+21,946K = (D+1) + 1,439K D+32,581K = (D+2) + 635K 2,821K = (D+2) + 875K Priceless!

15 November 30, 2012 Reza KazimiFour Hall Operation D+3 Conclusion It is possible to run all four CEBAF experimental halls simultaneously by changing the 5 th pass separator frequency and cutting the beam repetition rates for halls taking beam at the highest pass. The possibility of keeping the 500 MHz system alongside the 750 MHz system is considered but details need to be studied. An upgrade to the electron gun laser system will not only allow 4-hall operation but also provide an independently changeable low rep rate beam to each hall. The 750 MHz system would position us for future possibilities. The proposed design change can be accomplished within the existing schedule. A decision must be made before February.

16 November 30, 2012 Reza KazimiFour Hall Operation D+3 Acknowledgements Tom OrenPreparation of the Presentation Mike SpataHardware Needs, Cost, Schedule, … Haipeng WangRF and SRF Design John HansknechtGun Laser System Andrew Hutton Arne Freyberger Encouragement and Presentation MontPosing the Question

November 30, 2012 Reza KazimiFour Hall Operation D+3 17

18 November 30, 2012 Reza KazimiFour Hall Operation D+3 RF Separation – Existing (500 MHz)

19 November 30, 2012 Reza KazimiFour Hall Operation D+3 RF Separation – Proposed (750 MHz)

Accelerator Frequency 1500 MHz Accelerator Frequency 1500 MHz RF Separator Cavity 500 MHz RF Separator Cavity 500 MHz To Halls A,B,C Beam Halls A,B,C 5 th Pass Vertical Separation C C A A B B C C A A B B C C A A B B A A B B C C A A B B C C C C A A C C A A B B B B

21 August 2012 Reza KazimiFour Hall Operation D+3 System Timing Diagrams Timing signal reference from system oscillator (500 MHz) Laser pulses produced from first LiNb03 modulator (500 MHz) Digital output from Digitizer in Divide by 2 mode (250 MHz) Output of “one-shot” circuit when fed the 250MHz signal. (Notice that pulse width can actually be up to 2 ns wide and this would still work if phased properly) Laser pulses passing through the pulse picker LiNb03 modulator in Divide by 2 mode Digital output from Digitizer in Divide by 4 mode (125 MHz) Output of “one-shot” circuit when fed the 125MHz signal. (Notice that pulse width can actually be up to 2 ns wide and this would still work if phased properly) Laser pulses passing through the pulse picker LiNb03 modulator in Divide by 4 mode Diagrams are similar all the way to divide by 16 mode which will produce a MHz beam.

22 August 2012 Reza KazimiFour Hall Operation D+3 Laser Table Complete overview before changes: Seed Laser Pre-Amp Fiber 5W amp 500MHz rf input 1560nm to 780nm conversion Optics, attenuator, tune mode generator, etc HALL A Seed LaserPre-Amp Fiber 5W amp 500MHz rf input 1560nm to 780nm conversion Optics, attenuator, tune mode generator, etc HALL B Seed Laser Pre-Amp Fiber 5W amp 500MHz rf input 1560nm to 780nm conversion Optics, attenuator, tune mode generator, etc HALL C Beams to photo-cathode

23 August 2012 Reza KazimiFour Hall Operation D+3 Laser Table Upgrade that would add a stand-alone hall D laser. Seed LaserLiNb03 mod #1 LiNb03 mod #2 Pulse picker New control electronics Pre-Amp Fiber 5W amp 500MHz rf input 1560nm to 780nm conversion Optics, attenuator, tune mode generator, etc HALL A Seed LaserLiNb03 mod #1 LiNb03 mod #2 Pulse picker Pre-Amp Fiber 5W amp 500MHz rf input 1560nm to 780nm conversion Optics, attenuator, tune mode generator, etc HALL B Seed LaserLiNb03 mod #1 LiNb03 mod #2 Pulse picker Pre-Amp Fiber 5W amp 500MHz rf input 1560nm to 780nm conversion Optics, attenuator, tune mode generator, etc HALL C Seed LaserLiNb03 mod #1 LiNb03 mod #2 Pulse picker Pre-Amp Fiber 5W amp 500MHz rf input 1560nm to 780nm conversion Optics, attenuator, tune mode generator, etc HALL D New control electronics Beams to photo-cathode

24 August 2012 Reza KazimiFour Hall Operation D+3 Or... Install both! Install 500 MHz (D+2) and 750 MHz (D+3) separation systems. Has not been studied in detail but will likely work.  Aperture problems need to be investigated.  Cost considerations.

D+3 $2,581K D+3 $2,581K D+2 & D+3 $2,821K D+2 & D+3 $2,821K D+1 $507K D+1 $507K D+2 $1,946K D+2 $1,946K