AN INTRODUCTION TO THE FUNCTIONAL RENORMALIZATION GROUP: SCALING SOLUTIONS IN CONTINUOUS DIMENSION RICCARDO BEN ALÌ ZINATI 9 Giugno 2014 [Based on arXiv:1204.3877]
AN INTRODUCTION TO THE FUNCTIONAL RENORMALIZATION GROUP:!
SCALING SOLUTIONS IN CONTINUOUS DIMENSION
RICCARDO BEN ALÌ ZINATI
9 Giugno 2014
[Based on arXiv:1204.3877]
Wilson RG Functional RG ConclusionsOutline
Wilson Renormalization Group
Functional Renormalization Group
OUTLINE OF THE TALK
Effective Average action formalismExact RG equation
Derivative Expansion
Scaling solutions
Critical exponents
Z2 models
Z2 -models universality classes
WILSON’S RENORMALIZATION GROUP
Wilson RG Functional RG ConclusionsOutline Z2 models
Wilson RG Functional RG Conclusions
Close to a second order phase transition
⇠
a ⇠ ⇤�1 lattice spacing
correlation length
Outline Z2 models
Close to a second order phase transition
⇠
a ⇠ ⇤�1 lattice spacing
correlation length
At the critical point :
⇠ % 1 =) ⇠ � a ⇠ ⇤�1
Wilson RG Functional RG ConclusionsOutline
short distance physics is completely washed out!
Z2 models
At the critical point :
short distance physics is completely washed out!
⇠ % 1 =) ⇠ � a ⇠ ⇤�1
Wilson RG Functional RG ConclusionsOutline Z2 models
At the critical point :
short distance physics is completely washed out!
⇠ % 1 =) ⇠ � a ⇠ ⇤�1
WILSON’S IDEA
Built an effective theory for the long distance degrees of freedom
Wilson RG Functional RG ConclusionsOutline Z2 models
At the critical point :
short distance physics is completely washed out!
WILSON’S IDEA
⇠ % 1 =) ⇠ � a ⇠ ⇤�1
IMPLEMENTATION
Built an effective theory for the long distance degrees of freedom
RG Transformation = Coarse Graining + Rescaling
Wilson RG Functional RG ConclusionsOutline Z2 models
Z =X
{�i}
e�H({�i}, ~K) =X
{�B}
X
�i2B
e�H({�i}, ~K) ⌘X
{�B}
e�H({�B}, ~K0)
Kadanoff, Leo P. "Scaling laws for Ising models near Tc." Physics 2.263 (1966): 12.
RG Transformation = Coarse Graining + Rescaling
Wilson RG Functional RG ConclusionsOutline Z2 models
Z =
Z ⇤
D�(p) e�H[�, ~K] =
Z ⇤/s
D�<
"Z ⇤
⇤/s
D�> e�H[�<,�>, ~K]
#=
Z ⇤
D�0(p0) e�H[�0, ~K0]
Wilson, Kenneth G., and John Kogut. "The renormalization group and the ϵ expansion." Physics Reports 12.2 (1974): 75-199.
RG Transformation = Coarse Graining + Rescaling
Wilson RG Functional RG ConclusionsOutline Z2 models
!𝓡 ≔ 𝓒 ∘ 𝓢
Features of RG transformation:
Wilson RG Functional RG ConclusionsOutline Z2 models
!𝓡 ≔ 𝓒 ∘ 𝓢
Probes the system at different scales
Wilson RG Functional RG ConclusionsOutline
Features of RG transformation:
Z2 models
!𝓡 ≔ 𝓒 ∘ 𝓢
Probes the system at different scales
Preserves the partition function
Wilson RG Functional RG ConclusionsOutline
Features of RG transformation:
Z2 models
!𝓡 ≔ 𝓒 ∘ 𝓢
Probes the system at different scales
Maps Hamiltonians in Hamiltonians
Preserves the partition function
Wilson RG Functional RG ConclusionsOutline
Features of RG transformation:
Z2 models
!𝓡 ≔ 𝓒 ∘ 𝓢
Probes the system at different scales
Integrates out short distance degrees of freedom to obtain an effective theory for the long distance ones
Maps Hamiltonians in Hamiltonians
Preserves the partition function
Wilson RG Functional RG ConclusionsOutline
Features of RG transformation:
Z2 models
!𝓡 ≔ 𝓒 ∘ 𝓢
Probes the system at different scales
Preserves the partition function
Maps Hamiltonians in Hamiltonians
Integrates out short distance degrees of freedom to obtain an effective theory for the long distance ones
Generate a flow in the ( - dimensional) parameter space~K ! R( ~K) =: ~K 0
1
Wilson RG Functional RG ConclusionsOutline
Features of RG transformation:
Z2 models
!𝓡 ≔ 𝓒 ∘ 𝓢
Probes the system at different scales
Preserves the partition function
Maps Hamiltonians in Hamiltonians
Integrates out short distance degrees of freedom to obtain an effective theory for the long distance ones
Generate a flow in the ( - dimensional) parameter space~K ! R( ~K) =: ~K 0
1
Wilson RG Functional RG ConclusionsOutline
Features of RG transformation:
Z2 models
Critical Surface:
Mc := { ~K 2 ⌦ | ⇠ = 1}
Fixed Points~K⇤ = R( ~K⇤, s)
~K⇤~Kc
⇠ = 1
⌦physical line
~K ! R( ~K) =: ~K 0
Wilson RG Functional RG ConclusionsOutline Z2 models
Mc := { ~K 2 ⌦ | ⇠ = 1}
Fixed Points~K⇤ = R( ~K⇤, s)
~K⇤~Kc
⇠ = 1
⌦physical line
Hypothesis:
For points in a (finite or infinite) domain on the critical surface, the RG flow converges
to a fixed point
Wilson RG Functional RG ConclusionsOutline
Critical Surface:
Z2 models
~Kc~K⇤
⇠ = 1
⌦Mc := { ~K 2 ⌦ | ⇠ = 1}
Fixed Points~K⇤ = R( ~K⇤, s)
physical line
~K0
For points in a (finite or infinite) domain on the critical surface, the RG flow converges
to a fixed point
Wilson RG Functional RG ConclusionsOutline
Hypothesis:
Critical Surface:
Z2 models
~Kc~K⇤
⇠ = 1
⌦Mc := { ~K 2 ⌦ | ⇠ = 1}
Fixed Points~K⇤ = R( ~K⇤, s)
physical line
~K0
UNIVERSALITY
All the theories in the same basin of attraction
belongs to the same universality class
For points in a (finite or infinite) domain on the critical surface, the RG flow converges
to a fixed point
Wilson RG Functional RG ConclusionsOutline
Hypothesis:
Critical Surface:
Z2 models
FUNCTIONAL RENORMALIZATION GROUP
Wilson RG Functional RG ConclusionsOutline Z2 models
FUNCTIONAL RENORMALIZATION GROUP
Wilson RG Functional RG ConclusionsOutline
Main formulations
Wilson-Polchinski Approach
Polchinski, Joseph. "Renormalization and effective Lagrangians."
Nuclear Physics B 231.2 (1984): 269-295.
Effective Average Action Method
Wetterich, Christof. "Exact evolution equation for the effective potential."
Physics Letters B 301.1 (1993): 90-94.
Z2 models
Wilson RG Functional RG ConclusionsOutline
Wilson-Polchinski Approach
Polchinski, Joseph. "Renormalization and effective Lagrangians."
Nuclear Physics B 231.2 (1984): 269-295.
Effective Average Action Method
Wetterich, Christof. "Exact evolution equation for the effective potential."
Physics Letters B 301.1 (1993): 90-94.
Main formulations
FUNCTIONAL RENORMALIZATION GROUP
Z2 models
WHY FUNCTIONAL RENORMALIZATION GROUP ?
Wilson RG Functional RG ConclusionsOutline Z2 models
WHY FUNCTIONAL RENORMALIZATION GROUP ?
Wilson RG Functional RG ConclusionsOutline
Good convergence properties
Z2 models
Wilson RG Functional RG ConclusionsOutline
Good convergence properties
Recover known results -expansion, loop expansion,…✏
WHY FUNCTIONAL RENORMALIZATION GROUP ?
Z2 models
Wilson RG Functional RG ConclusionsOutline
Good convergence properties
Recover known results -expansion, loop expansion,…✏
New approximation schemes: go beyond perturbation theory
WHY FUNCTIONAL RENORMALIZATION GROUP ?
Z2 models
Wilson RG Functional RG ConclusionsOutline
Good convergence properties
Recover known results -expansion, loop expansion,…✏
Computation valid for any dimension d
New approximation schemes: go beyond perturbation theory
WHY FUNCTIONAL RENORMALIZATION GROUP ?
Z2 models
Wilson RG Functional RG ConclusionsOutline
Good convergence properties
Recover known results -expansion, loop expansion,…✏
Computation valid for any dimension d
New approximation schemes: go beyond perturbation theory
Find systematically all possible non-perturbative massless continuum limits for QFTs
WHY FUNCTIONAL RENORMALIZATION GROUP ?
Z2 models
Effective Action
Z [J ] =
ZD� e�S[�]+
Rd
dx �(x)J(x)Partition Function
Wilson RG Functional RG ConclusionsOutline Z2 models
Effective Action
Z [J ] =
ZD� e�S[�]+
Rd
dx �(x)J(x)Partition Function
W [J ] = logZ [J ]Free Energy
Wilson RG Functional RG ConclusionsOutline Z2 models
Effective Action
Z [J ] =
ZD� e�S[�]+
Rd
dx �(x)J(x)Partition Function
�W
�J(x)= h�(x)ic =: '(x)W [J ] = logZ [J ]Free Energy
Wilson RG Functional RG ConclusionsOutline Z2 models
Effective Action
Z [J ] =
ZD� e�S[�]+
Rd
dx �(x)J(x)Partition Function
�W
�J(x)= h�(x)ic =: '(x)W [J ] = logZ [J ]Free Energy
� ['] = �W [J ] +
Zd
dx '(x)J(x)Gibbs Free Energy
Wilson RG Functional RG ConclusionsOutline Z2 models
Effective Action
Partition Function
�W
�J(x)= h�(x)ic =: '(x)W [J ] = logZ [J ]Free Energy
� ['] = �W [J ] +
Zd
dx '(x)J(x)Gibbs Free Energy
More transparent physical interpretation
Generates 1PI Graphs
Wilson RG Functional RG ConclusionsOutline
Z [J ] =
ZD� e�S[�]+
Rd
dx �(x)J(x)
Z2 models
Built a one parameter family of functionals interpolating between bare action
and effective actionS
�
Effective Average Action Idea
Wilson RG Functional RG ConclusionsOutline Z2 models
Built a one parameter family of functionals interpolating between bare action
and effective actionS
�
Effective Average Action Idea
Wilson RG Functional RG ConclusionsOutline
How to do it?
Z2 models
Effective Average Action
e��['] =
ZD� e�S['+�]+
Rd
d
x
���'(x)�(x)
Wilson RG Functional RG ConclusionsOutline Z2 models
Add the (IR) cutoff term
e��['] =
ZD� e�S['+�]+
Rd
d
x
���'(x)�(x)
e��k
['] :=
ZD� e�S['+�]��S
k
[�]+Rd
d
x
��k
�'(x)�(x)
Wilson RG Functional RG ConclusionsOutline
Effective Average Action
Effective Average Action
Z2 models
e��['] =
ZD� e�S['+�]+
Rd
d
x
���'(x)�(x)
e��k
['] :=
ZD� e�S['+�]��S
k
[�]+Rd
d
x
��k
�'(x)�(x)
Γ =S≡ k �k=⇤ ['] = S[� = ']
no fluctuation has been integrated out
Add the (IR) cutoff term
Wilson RG Functional RG ConclusionsOutline
Effective Average Action
Z2 models
e��['] =
ZD� e�S['+�]+
Rd
d
x
���'(x)�(x)
e��k
['] :=
ZD� e�S['+�]��S
k
[�]+Rd
d
x
��k
�'(x)�(x)
�k=0 ['] = � [']
�k=⇤ ['] = S[� = ']
no fluctuation has been integrated out
all fluctuations are integrated out
Γk
k
Add the (IR) cutoff term
Wilson RG Functional RG ConclusionsOutline
Effective Average Action
Z2 models
Universal properties won’t depend on the cutoff chosen!
�Sk [�] =1
2
Zddq
(2⇡)d�(�q)Rk(q)�(q)The (IR) cutoff term
Rmassk (q) = k2
Ropt
k (q) = (k2 � q)✓(k2 � q)
Rexp
k (q) =q
eq/k2 � 1
Rk(q)
q
Wilson RG Functional RG ConclusionsOutline Z2 models
Take the scale derivative of
EXACT RG EQUATION FOR THE EEA
Wetterich, Christof. "Exact evolution equation for the effective potential." Physics Letters B 301.1 (1993): 90-94.
@t�k ['] =1
2Tr
⇢h�(2)k ['] +Rk
i�1@tRk
�
e��k
['] :=
ZD� e�S['+�]��S
k
[�]+Rd
d
x
��k
�'(x)�(x)
Wilson RG Functional RG ConclusionsOutline Z2 models
Wilson RG Functional RG ConclusionsOutline
functional integro-differential non-linear exact equation
EXACT RG EQUATION FOR THE EEA
one-loop structure
IR and UV finite
=1
2@t�k['] =
1
2Tr
⇢h�(2)k ['] +Rk
i�1@tRk
�
Z2 models
How to solve it?
Wilson RG Functional RG ConclusionsOutline Z2 models
How to solve it?
Vertex ExpansionExpand in powers of the field
Iterative solutionPick a seed and solve by iteration
Wilson RG Functional RG ConclusionsOutline
Derivative ExpansionExpand in powers of momenta
Z2 models
How to solve it?
Vertex ExpansionExpand in powers of the field
Iterative solutionPick a seed and solve by iteration
Derivative ExpansionExpand in powers of momenta
Wilson RG Functional RG ConclusionsOutline Z2 models
Derivative ExpansionExpand in powers of momenta
�k['] =
Zddx
Vk(') +
1
2Zk(') (@')
2�+O(@4)
Project the exact FRG equation to obtain a set of coupled p.d.e. involving the running functions:
@tVk(')
@tZk(')
...
Wilson RG Functional RG ConclusionsOutline Z2 models
Make a truncation Ansatz
�k['] =
Zd
dx
Vk(') +
1
2(@')2
�
Derivative Expansion: LPA
Nicoll, J. F., T. S. Chang, and H. E. Stanley. "Approximate renormalization group based on the Wegner-Houghton differential generator." Physical Review Letters 33.9 (1974): 540.
Wilson RG Functional RG ConclusionsOutline Z2 models
Make a truncation Ansatz
�k['] =
Zd
dx
Vk(') +
1
2(@')2
�
Calculate the Hessian
�
2�k[']
�'(x)�'(x0)=
⇥�@
2 + V
00k (�)
⇤�(x� x
0)
Derivative Expansion: LPA
Nicoll, J. F., T. S. Chang, and H. E. Stanley. "Approximate renormalization group based on the Wegner-Houghton differential generator." Physical Review Letters 33.9 (1974): 540.
Wilson RG Functional RG ConclusionsOutline Z2 models
Make a truncation Ansatz
�k['] =
Zd
dx
Vk(') +
1
2(@')2
�
Calculate the Hessian
�
2�k[']
�'(x)�'(x0)=
⇥�@
2 + V
00k (�)
⇤�(x� x
0)
Insert into the ERG equation
@t�k['] = Tr@tRk(�@2)
�@2 + V 00k (') +Rk(�@2)
Derivative Expansion: LPA
Nicoll, J. F., T. S. Chang, and H. E. Stanley. "Approximate renormalization group based on the Wegner-Houghton differential generator." Physical Review Letters 33.9 (1974): 540.
Wilson RG Functional RG ConclusionsOutline Z2 models
Make a truncation Ansatz
�k['] =
Zd
dx
Vk(') +
1
2(@')2
�
Calculate the Hessian
�
2�k[']
�'(x)�'(x0)=
⇥�@
2 + V
00k (�)
⇤�(x� x
0)
Insert into the ERG equation
@t�k['] = Tr@tRk(�@2)
�@2 + V 00k (') +Rk(�@2)
and project
@tVk(') =1
2(4⇡)d/2�(d/2)
Z 1
0dz zd/2�1 @tRk(z)
�z + V 00k (') +Rk(z)
Derivative Expansion: LPA
Wilson RG Functional RG ConclusionsOutline Z2 models
Choose a cut off shape function to obtain an explicit solution
@tVk(') = cdkd
1 +V 00k (')k2
Derivative Expansion: LPA
Wilson RG Functional RG ConclusionsOutline Z2 models
Choose a cut off shape function to obtain an explicit solution
@tVk(') = cdkd
1 +V 00k (')k2
Introduce dimensionless variables to implement scaling
' = kd/2�1' Vk(') = kdVk(')
to obtain the p.d.e. for the effective dimensionless potential
@tVk(') = �d Vk(') +
✓d
2� 1
◆' V 0
k(') +cd
1 + V 00k (')
Derivative Expansion: LPA
S
Wilson RG Functional RG ConclusionsOutline Z2 models
Choose a cut off shape function to obtain an explicit solution
@tVk(') = cdkd
1 +V 00k (')k2
' = kd/2�1' Vk(') = kdVk(')
to obtain the p.d.e. for the effective dimensionless potential
@tVk(') = �d Vk(') +
✓d
2� 1
◆' V 0
k(') +cd
1 + V 00k (')
Derivative Expansion: LPA
Wilson RG Functional RG ConclusionsOutline
Introduce dimensionless variables to implement scaling S
Z2 models
@tVk(') = �d Vk(') +
✓d
2� 1
◆' V 0
k(') +cd
1 + V 00k (')
Scaling Solutions Z2 models LPA
Wilson RG Functional RG ConclusionsOutline Z2 models
@tVk(') = �d Vk(') +
✓d
2� 1
◆' V 0
k(') +cd
1 + V 00k (')
Ordinary Differential Equation
Scaling solution
@tV⇤(') = 0
�dV⇤(') +d� 2
2'V 0
⇤(') + cd1
1 + V 00⇤ (')
= 0
Wilson RG Functional RG ConclusionsOutline
Scaling Solutions Z2 models LPA
Z2 models
�dV⇤(') +d� 2
2'V 0
⇤(') + cd1
1 + V 00⇤ (')
= 0
V 0⇤(0) = 0
V⇤(0) =cd/d
1 + V 00⇤ (0)
V 00⇤ (0) =: �
(Initial conditions
Z2 symmetry
Scaling Solutions Z2 models LPA
Wilson RG Functional RG ConclusionsOutline Z2 models
�dV⇤(') +d� 2
2'V 0
⇤(') + cd1
1 + V 00⇤ (')
= 0
V 0⇤(0) = 0
V 00⇤ (0) =: �
(Initial conditions
Singularities
'ds(�) := {' | V (') % 1, 8 {d,�}}
Search for universality classes Plot the function ! 'ds(�)
Scaling Solutions Z2 models LPA
Wilson RG Functional RG ConclusionsOutline
Requiring the potential to be well defined 8' 2 R
Z2 models
Wilson RG Functional RG ConclusionsOutline
'ds(�)
�
Universality classes appear as “spikes”
Z2 models
Wilson RG Functional RG ConclusionsOutline
'ds(�)
�
Ising
Z2 models
Wilson RG Functional RG ConclusionsOutline
'ds(�)
�
Ising
Ising Tri-critical
Z2 models
Wilson RG Functional RG ConclusionsOutline
'ds(�)
�
Ising Tri-critical
Ising Tetra-critical
Ising
Z2 models
Wilson RG Functional RG ConclusionsOutline
'ds(�)
�
'ds(�)
d=2.01 Toward CFT minimal models!
Z2 models
Scaling Solutions Z2 models LPA’
�dV⇤(') +d� 2 + ⌘
2'V 0
⇤(') + cd1� ⌘
d+2
1 + V 00⇤ (')
= 0
⌘k = cd
hV 000k ('0)
i2
h1 + V 00
k ('0)i4
Add the anomalous dimension!
Solve iteratively
Wilson RG Functional RG ConclusionsOutline Z2 models
Wilson RG Functional RG ConclusionsOutline
0.4
0.1
0.2
0.3
3.02.82.62.42.2
⌘i
d
Anomalous dimension of the first five multi-critical scaling solution as a function of d.
⌘i
Z2 models
Wilson RG Functional RG ConclusionsOutline
Anomalous dimension of the first ten multi critical scaling solution in dimension d=2.
⌘i
@2O( )LPA’
CFT0.4
0.1
0.2
0.3
2 4 6 8 10
⌘i
i
Z2 models
Critical exponents LPA
@tVk(') = �d Vk(') +
✓d
2� 1
◆' V 0
k(') +cd
1 + V 00k (')
Wilson RG Functional RG ConclusionsOutline Z2 models
@tVk(') = �d Vk(') +
✓d
2� 1
◆' V 0
k(') +cd
1 + V 00k (')
Vk(') = �0 +�2
2!'2 +
�4
4!'4 +
�6
6!'6 + . . .Expand
@tVk @t�2n
Wilson RG Functional RG ConclusionsOutline
Critical exponents LPA
Z2 models
@tVk(') = �d Vk(') +
✓d
2� 1
◆' V 0
k(') +cd
1 + V 00k (')
Vk(') = �0 +�2
2!'2 +
�4
4!'4 +
�6
6!'6 + . . .Expand
�2n = @t�2n
All the beta functions for the running couplings can be extracted
�2n =(2n)!
n!
@n
@('2)n@tVk(')
�����'=0
The effective potential is the generating function for Beta functions
Wilson RG Functional RG ConclusionsOutline
Critical exponents LPA
Z2 models
Mnm =@�2n
@�2m
�����⇤
Compute stability matrix
Eigenvalues ⇤1(d) < 0 < ⇤2(d) < ⇤3(d) < . . .
⌫(d) = � 1
⇤1(d)Correlation length critical exponent
Wilson RG Functional RG ConclusionsOutline
Critical exponents LPA
Z2 models
↵+ 2� + � = 2
↵+ �� + � = 2
⌫(2� ⌘) = �
↵+ ⌫d = 2
Scaling laws
Wilson RG Functional RG ConclusionsOutline Z2 models
⌘⌫↵��
�
LPA’ Exact LPA’ World best
0,436 0,25 0,11 0,036
1,05 1 0,65 0,63
-0,11 0 0,06 0,11
0,23 0,125 0,36 0,33
1,65 1,75 1,22 1,24
10,17 15 4,60 4,79
d=2 d=3
Belavin Alexander A., Alexander M. Polyakov, and Alexander B. Zamolodchikov. "Infinite conformal symmetry in two-dimensional quantum field theory." Nuclear Physics B 241.2 (1984): 333-380.
Critical exponents for the Ising universality class in d=2 and in d=3 compared to exact result and world best estimates
Pelissetto Andrea, and Ettore Vicari. "Critical phenomena and renormalization-group theory." Physics Reports 368.6 (2002): 549-727.
Wilson RG Functional RG ConclusionsOutline Z2 models
Follow, continuously with d, the evolution of RG fixed points through the functional theory space
of effective potentials
CONCLUSIONS
Wilson RG Functional RG ConclusionsOutline Z2 models
Follow, continuously with d, the evolution of RG fixed points through the functional theory space
of effective potentials
Validation of the correspondence between Landau-Ginsburg actions and minimal models of CFT
Wilson RG Functional RG ConclusionsOutline
CONCLUSIONS
Z2 models
Follow, continuously with d, the evolution of RG fixed points through the functional theory space
of effective potentials
Validation of the correspondence between Landau-Ginsburg actions and minimal models of CFT
LPA captured qualitatively all possible critical behaviour associated with Z2-simmetry in any d 2.�
Wilson RG Functional RG ConclusionsOutline
CONCLUSIONS
Z2 models
Follow, continuously with d, the evolution of RG fixed points through the functional theory space
of effective potentials
Validation of the correspondence between Landau-Ginsburg actions and minimal models of CFT
LPA captured qualitatively all possible critical behaviour associated with Z2-simmetry in any d 2.
LPA’ quantitatively reproduced well the known results for critical exponents
�
Wilson RG Functional RG ConclusionsOutline
CONCLUSIONS
Z2 models
THANK YOU
Wilson RG Functional RG ConclusionsOutline Z2 models
MAIN REFERENCES
Wilson RG Functional RG ConclusionsOutline
Berges Jürgen, Nikolaos Tetradis, and Christof Wetterich. "Non-perturbative renormalization flow in quantum field theory and statistical physics."
Physics Reports 363.4 (2002): 223-386.
Delamotte Bertrand. "An introduction to the nonperturbative renormalization group."
Renormalization Group and Effective Field Theory Approaches to Many-Body Systems. Springer Berlin Heidelberg, 2012. 49-132.
Codello Alessandro. "Scaling solutions in a continuous dimension."
Journal of Physics A: Mathematical and Theoretical 45.46 (2012): 465006.
Morris Tim R. "Elements of the continuous renormalization group."
arXiv hep-th/9802039 (1998).
Mussardo, Giuseppe. Statistical field theory.
Oxford Univ. Press, 2010.
Z2 models