numerical studies of universality in few-boson systems javier von stecher department of physics and...
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![Page 1: Numerical Studies of Universality in Few-Boson Systems Javier von Stecher Department of Physics and JILA University of Colorado Probable configurations](https://reader030.vdocument.in/reader030/viewer/2022032800/56649d435503460f94a1fb41/html5/thumbnails/1.jpg)
Numerical Studies of Universality in Few-Boson Systems
Numerical Studies of Universality in Few-Boson Systems
Javier von Stecher Department of Physics and JILA University of Colorado
Probable configurations of a weakly-bound four-boson state.
Acknowledgements:Doerte BlumeSeth RittenhouseNirav MehtaNSF
In collaboration withChris H. GreeneJose P. D’Incao
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How does Efimov physics and How does Efimov physics and universality extends beyond universality extends beyond
three bodies?three bodies?
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Outline:Outline:
Universality in four-boson systems
Numerical formulation (CG and CGH) Four-bosons predictions
Extension to larger systems
Model Hamiltonian Cluster states
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Outline:Outline:
Universality in four-boson systems
Numerical formulation (CG and CGH) Four-bosons predictions
Extension to larger systems
Model Hamiltonian Cluster states
![Page 5: Numerical Studies of Universality in Few-Boson Systems Javier von Stecher Department of Physics and JILA University of Colorado Probable configurations](https://reader030.vdocument.in/reader030/viewer/2022032800/56649d435503460f94a1fb41/html5/thumbnails/5.jpg)
Solving the Schrödinger equationSolving the Schrödinger equation
Hamiltonian:
Four-body Formulation
model interactions:
rr
V(r)
V(r) dd00
a<0a>0
VV00
aa
dimer energydimer energyscattering scattering lengthlength
-
or combinations of Gaussians
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Analytical form of matrix elements (accurate and fast). Efficient Optimization: Stochastical variational method Good for bound states. Difficult to describe scattering properties
Correlated Gaussian basis set expansion:Correlated Gaussian basis set expansion:
r12
r13r24
r34
r14r23
1 2
34
• remove CM and set L=0
Symmetrization: spin statistic
• basis functions:
Four-body Formulation
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Hyperspherical representation:Hyperspherical representation:
Coupled 1D equations…solved at fixed R.
Use correlated Gaussian to expand channel functionsUse correlated Gaussian to expand channel functions
Divide and conquer:
Find efficient way to evaluate matrix elements
R
Accurate description of four-body systems!!Accurate description of four-body systems!!
R: overall size
(collective motion)
typical potential curves
Four-body Formulation J. von Stecher, C. H. Greene PRA (2009)
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1+1+1+1
2+1+1
2+2
3+1
3+1
Hyperspherical PictureHyperspherical Picture
RR
v
v
Fragmentation thresholds
All particles close together:Bound and quasi-bound states
Interaction region
U(R
U(R
)
……for scattering properties.for scattering properties.
Four-body Formulation
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s0=2.0096 (CG) s0=2.0092 (CGH)
Universality arguments predict that the hyperspherical potential curves are of the type (Tan, Werner & Castin, …):
J. von Stecher, C. H. Greene PRA (2009)
J. von Stecher, D. Blume, C. H. Greene PRL 2007, PRA 2007, 2008
S.Y. Chang, and G. F. Bertsch PRA (R) (2007)
I. Stetcu, B. Barrett, U. van Kolck, J. Vary. PRA (2007)
Y. Alhassid, G. F. Bertsch, and L. Fang PRL (2008)
…..
Trap system predictions:
Four fermion system at unitarityFour fermion system at unitarity
Appropriate framework to analyze universality
D.S. Petrov, C. Salomon, G.V. Shlyapnikov PRL (2004)
Connection to trapped system:trap
frequency
Predictions:
See also: J. P. D’Incao et al PRA (2009)
Hyperspherical PictureHyperspherical Picture……for studying universalityfor studying universality
Four-body Formulation
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Outline:Outline:
Universality in four-boson systems
Numerical formulation (CG and CGH) Four-bosons predictions
Extension to larger systems
Model Hamiltonian Cluster states
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Four-BosonsFour-Bosons
, …
, …
, …
3 body3 body
4 body4 body
Efimov scaling
Efimov scaling
Two four-body states
same scaling relations!!!
Universality in four bosonsUniversality in four bosons
a=
J. von Stecher, J. P. D’Incao and C. H. Greene, Nat. Phys. (2009)
In agreement with Hammer & Platter EJPA (2007)(Hammer presentation)
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RR RR
3 bodies3 bodies 4 bodies4 bodies
Four-BosonsFour-Bosons
Hyperspherical Picture (a=Hyperspherical Picture (a=))
v
v
v
Four-body potential curves follow the same scaling of the Efimov states !!!
Four-body physics is universal!!
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RR RR
3 bodies3 bodies 4 bodies4 bodies
Four-BosonsFour-Bosons
Hyperspherical Picture (a=Hyperspherical Picture (a=))
v
v
v
Four-body potential curves follow the same scaling of the Efimov states !!!
Four-body physics is universal!!
Three-body parameter:
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RR RR
3 bodies3 bodies 4 bodies4 bodies
Four-BosonsFour-Bosons
Hyperspherical Picture (a=Hyperspherical Picture (a=))
v
v
v
Four-body potential curves follow the same scaling of the Efimov states !!!
Four-body physics is universal!!
Three-body parameter:
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Four-BosonsFour-Bosons
Four-body statesFour-body states
a=
J. von Stecher, J. P. D’Incao and C. H. Greene, Nat. Phys. (2009)
Hammer & Platter prediction:
Agreement with Hammer & Platter (2007)
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Four-BosonsFour-Bosons
v
Spectrum: Extended Efimov plotSpectrum: Extended Efimov plot
1/a
J. von Stecher, J. P. D’Incao and C. H. Greene, Nat. Phys. (2009)
Calculations at more than 500 scattering lengths!!!
atom-trimer thresholds(green lines)
four-body states(black lines)
dimer-dimer threshold(red lines)
dimer-two atoms threshold(red lines)
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v
~1/a
Four-BosonsFour-Bosons
Universality away from unitarityUniversality away from unitarity
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v
~1/a
Four-BosonsFour-Bosons
Universality away from unitarityUniversality away from unitarity
v
1/a
Ener
gy
a*4b2 a*
3ba*4b1
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v
~1/a
Four-BosonsFour-Bosons
Universality away from unitarityUniversality away from unitarity
v
1/a
Ener
gy
a*4b2 a*
3ba*4b1
v
1/a
a*ad
a*dd,1
a*dd,2
acdd
Ener
gy
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Four-BosonsFour-Bosons
Universality away from unitarityUniversality away from unitarity
v
1/a
Ener
gy
a*4b2 a*
3ba*4b1
a<0
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Four-BosonsFour-Bosons
Universality away from unitarityUniversality away from unitarity
v
1/a
Ener
gy
a*4b2 a*
3ba*4b1
v
1/a
a*ad
a*dd,1
a*dd,2
acdd
Ener
gy
Universal four-body resonances in ultracold atomic and molecular gases J. P. D’Incao
This afternoon:Important for collisional propertiesImportant for collisional properties Experimental observationsExperimental observations
a>0a<0
(Innsbruck, LENS)
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Outline:Outline:
Universality in four-boson systems
Numerical formulation (CG and CGH) Four-bosons predictions
Extension to larger systems
Model Hamiltonian Cluster states
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N-BosonsN-Bosons
How to extend the analysis How to extend the analysis of universality to larger of universality to larger
systems?systems?
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N-BosonsN-Bosons
Helium and spin-polarized tritium:similar behavior
Extension to larger systemsExtension to larger systems
Other studies:
Lewerenz, JCP (1997).Blume & Greene, JCP(2000).Hanna & Blume, PRA (2006).…
Blume et al., PRL(2002)
How many parameters are needed to describe N-boson systems?
Hammer & Platter, EPJA (2007).
• Linear correlations between cluster energies (like Tjon lines)
Hanna & Blume, PRA (2006):
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Outline:Outline:
Universality in four-boson systems
Numerical formulation (CG and CGH) Four-bosons predictions
Extension to larger systems
Model Hamiltonian Cluster states
![Page 26: Numerical Studies of Universality in Few-Boson Systems Javier von Stecher Department of Physics and JILA University of Colorado Probable configurations](https://reader030.vdocument.in/reader030/viewer/2022032800/56649d435503460f94a1fb41/html5/thumbnails/26.jpg)
short-range physics
3 bodies3 bodies
Universal region
Model HamiltonianModel Hamiltonian
N-BosonsN-Bosons
Hyperspherical potential at unitatityHyperspherical potential at unitatity
dilute and weakly bound ~ universal
controlled by short-range physics
J. von Stecher arXiv:0909.4056 (2009)
RR
Goal: construct a minimal Hamiltonian that would lead to a
“universal ground state”.
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short-range physics
3 bodies3 bodies
Universal region
Model HamiltonianModel Hamiltonian
N-BosonsN-Bosons
Hyperspherical potential at unitatityHyperspherical potential at unitatity
dilute and weakly bound ~ universal !!
RC
Lowest state is universal !!!Lowest state is universal !!!
J. von Stecher arXiv:0909.4056 (2009)
Goal: construct a minimal Hamiltonian that would lead to a
“universal ground state”.
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Model HamiltonianModel Hamiltonian
N-BosonsN-Bosons
controls three-body physics:3-body parameter
controls two-body physics:scattering length
Many-body Hamiltonian:Many-body Hamiltonian:
J. von Stecher arXiv:0909.4056 (2009)
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Model HamiltonianModel Hamiltonian
N-BosonsN-Bosons
Many-body Hamiltonian:Many-body Hamiltonian:
3 bodies3 bodies2 bodies2 bodies
rrijij
(r(r
ijij))
Bethe Peierls boundary condition
Two parameters (a and Rc) to independently control two and three-body physics.
U(R
U(R
)
RC
J. von Stecher arXiv:0909.4056 (2009)
Hard core three-body potential
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N-BosonsN-Bosons
Numerical methodsNumerical methods
J. von Stecher arXiv:0909.4056 (2009)
Correlated Gaussian basis set expansion up to N=6.
Diffusion Monte Carlo simulations up to N=13.
• Gaussian potential for two and three-body interactions
• Hard Wall 3-body potential and an attractive square 2-body potential
• Trial wave function:
3-body correlations
2-body correlations
HR correlations
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Outline:Outline:
Universality in four-boson systems
Numerical formulation (CG and CGH) Four-bosons predictions
Extension to larger systems
Model Hamiltonian Cluster states
![Page 32: Numerical Studies of Universality in Few-Boson Systems Javier von Stecher Department of Physics and JILA University of Colorado Probable configurations](https://reader030.vdocument.in/reader030/viewer/2022032800/56649d435503460f94a1fb41/html5/thumbnails/32.jpg)
N-BosonsN-Bosons
Weakly-bound ClustersWeakly-bound Clusters
Universal description: (just from dimensional analysis)
Universal functionUniversal function
Numerical predictions:
J. von Stecher arXiv:0909.4056 (2009)
Comparison with other predictions
Comparison between CG and DMC
At least one N-body cluster state for each Efimov trimer!!
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“Super” Borromean states
Linear Correlations (Tjon lines):
N-body resonant enhancement of losses:
N-BosonsN-Bosons
Weakly-bound ClustersWeakly-bound Clusters
J. von Stecher arXiv:0909.4056 (2009)
Position of five-body resonance:Semi-Classical Methods and N-Body Recombination
S. Rittenhouse
This afternoon:
Properties:Properties:
Positions of resonances
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N-BosonsN-Bosons
Dilute ClustersDilute Clusters
Pair correlation functionPair correlation function
Trayectories extracted from Quantum Monte Carlo simulations
Sphere radius: ~ 4r0 ~Rc
Five-body cluster state:Five-body cluster state:
rm~ 7Rc ~ 30 r0
~ 2Rc
N=3
N=6
J. von Stecher arXiv:0909.4056 (2009)
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RR
N bodiesN bodies
N-BosonsN-Bosons
Hyperspherical PictureHyperspherical Picture
Helium clustersHelium clustersMonte Carlo + Hyperspherical
D. Blume & C. H. Greene, JCP 2001
3+13+14+14+1
5+15+1
1+1+11+1+1
Potential curves scale with size and energy of cluster states All clusters follow Efimov scaling relations
J. von Stecher arXiv:0909.4056 (2009)
……sketching potentialssketching potentials
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• Extract width of four-body states
• Different species or/and spin statistic?– Universality?– Four-body states?
• Model Hamiltonian– with Quantum Monte Carlo
• Cluster states– Large N limit
Outlook:Outlook:
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Energy per particle at unitarityEnergy per particle at unitarity
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Four-BosonsFour-Bosons
Four-body statesFour-body states
a=
J. von Stecher, J. P. D’Incao and C. H. Greene, Nat. Phys. (2009)
Hammer & Platter prediction:
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Four-BosonsFour-Bosons
Four-body statesFour-body states
Weakly bound atom trimer state:Large and positive atom-trimer scattering length
Agreement with Hammer & Platter (2007)
a=
J. von Stecher, J. P. D’Incao and C. H. Greene, Nat. Phys. (2009)
atom- trimer correlation
trimer correlation
Pair correlationsPair correlations
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a>0
a<0
Blue: atom-trimerRed: dimer-dimerGreen dimer-2-atoms
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Four-BosonsFour-Bosons
Deviations from universalityDeviations from universality
J. von Stecher, J. P. D’Incao and C. H. Greene, Nat. Phys. (2009)
Deviations:2nd order four-body corrections or numerical limitations?
Non universal Universal
Scattering length ratios for a<0 depends weakly on nonuniversal effects!!
less than 5%deviations
Different potentials Different Efimov states
Universal
Non Universal
Testing universality: