non-commutative solitons and integrable equationshamanaka/040120t.pdf · 2004-01-17 · relativity...
TRANSCRIPT
Relativity Seminar at Oxford
Non-commutative Solitonsand Integrable Equations
Masashi HAMANAKA(Tokyo U. present)
(Nagoya U. from Feb. 2004)
MH, ``Commuting Flows andConservation Laws for NC Lax Hierarches,’’ [hep-th/0311206]cf. MH,``Noncommutative Solitonsand D-branes,’’ Ph.D thesis [hepth/0303256]
1. Introduction• Noncommutative spaces are
defined by noncommutativityof spatial coordinates:
This looks like CCR in QM:
``space-space uncertainly relation’’
Resolution of singulality( New physical objects)
e.g. resolution of small instanton singularity( U(1) instantons)
ijji ixx θ=],[
hipq =],[
NC gauge theories(real physics)
Commutative gauge theories in background of magnetic fields
• Gauge theories are realized on D-branes which are solitons in string theories
• In this contect, NC solitons are (lower-dim.) D-branesAnalysis of NC solitons (easy)
Analysis of D-branesVarious successful applicationse.g. confirmation of Sen’sconjecture on decay of D-branes
NC soliton theories are worthwhile !
Soliton equations indiverse dimensions
4 Anti-Self-Dual Yang-Mills eq.(instantons)
2(+1)
KP eq. BCS eq. 2-dim. AKNS system …
3 Bogomol’nyi eq.(monopoles)
1(+1)
KdV eq. mKdV eqBoussinesq eq.NLS eq. Burgers eq. sine-Gordon eq.Sawada-Kotera eq.…
µνµν FF ~−=
Dim. of space
NC extension (Successful)
NC extension (This talk)
NC extension(Successful)
NC extension(This talk)
Ward’s observation:Almost all integrableequations are reductions of the ASDYM eqs.
ASDYM eq.
KP eq. BCS eq. KdV eq. Boussinesq eq.
NLS eq. mKdV eq. sine-Gordon eq.
Burgers eq. …(Almost all ! )
Reductions
e.g. [Mason&Woodhouse]
R.Ward,Phil.Trans.Roy.Soc.Lond.A315(’85)451
NC Ward’s observation: Almost all NC integrableequations are reductions of the NC ASDYM eqs.
MH&K.Toda,PLA316(‘03)77[hepth/0211148]
NC ASDYM eq.
NC KP eq. NC BCS eq. NC KdV eq. NC Boussinesq eq.
NC NLS eq. NC mKdV eq. NC sine-Gordon eq.NC Burgers eq. …
(Almost all !?)
Reductions
Successful
Successful?
Sato’s theory may answer
Plan of this talk
1. Introduction2. NC Gauge Theory3. NC Sato’s Theory4. Conservation Laws5. Conclusion and Discussion
2. NC Gauge Theory• NC gauge theories are equivalent
to ordinary gauge theories in background of magnetic fields.
• They are obtained from ordinary commutative gauge theories by replacing products of fields with star-products.
• The star product:
)(2
exp)(:)()( xgixfxgxf jiij ⎟
⎠⎞
⎜⎝⎛ ∂∂=∗
rsθ
)()()(2
)()( 2θθ Oxgxfixgxf jiij +∂∂+=
A deformed product
hgfhgf ∗∗=∗∗ )()( Associative
ijijjiji ixxxxxx θ=∗−∗=∗ :],[ NC !
(Ex.) 4-dim. (Euclidean) G=U(N) Yang-Mills theory
• Action
• Eq. Of Motion:
• BPS eq. (=(A)SD eq.)
∫= µνµν FFTrxdS 4
( )( )[ ]µνµνµνµν
µνµνµνµν
FFFFTrxd
FFFFTrxd~2~
~~
24
4
±=
+=
∫∫
m
]),[:( νµµννµµν AAAAF +∂−∂=
0]],[,[ =µνν DDD
µνµν FF ~±= instantons
0,0212211==+ zzzzzz FFF
(Ex.) 4-dim. NC (Euclidean) G=U(N) Yang-Mills theory
(All products are star products)
• Action
• Eq. Of Motion:
• BPS eq. (=(A)SD eq.)
∫ ∗= µνµν FFTrxdS 4
( )( )[ ]µνµνµνµν
µνµνµνµν
FFFFTrxd
FFFFTrxd~2~
~~
24
4
∗±=
∗+∗=
∗∫∫
m
0]],[,[ =∗∗µνν DDD
µνµν FF ~±= NC instantons
0,0212211==+ zzzzzz FFF
)],[:( ∗+∂−∂= νµµννµµν AAAAF
Don’t omit evenfor G=U(1)
))()1(( ∞≅UUQ
ADHM construction of instantonsAtiyah-Drinfeld-Hitchin-Manin, PLA65(’78)185
ADHM eq. (G=``U(k)’’): k times k matrix eq.
0],[0],[],[
21
2211
=+=−++ ∗∗∗∗
IJBBJJIIBBBB
kNNk
kk
JIB
××
×
:,:,:2,1
NNA ×:µ
0
0
21
2211
=
=+
zz
zzzz
F
FF
ASD eq. (G=U(N), C2=-k): N times N PDE
ADHM data
Instatntons
1:1 k D0-branes
BPS
N D4-branes
BPS
ADHM construction of BPST instantons (N=2,k=1)
ADHM eq. (G=``U(1)’’)
0],[0],[],[
21
2211
=+=−++ ∗∗∗∗
IJBBJJIIBBBB
⎟⎠⎞
⎜⎝⎛
===ρ
ρα0
( ),0,,2,12,1 JIB
position size
)(222
2
22
)(
))((2,
)()( −
−
+−=
+−−
= µνµνµν
ν
µ ηρ
ρρ
ηbx
iFbxbxi
A
0→ρASD eq. (G=U(2), C2=-1)
singular
0
0
21
2211
=
=+
zz
zzzz
F
FFM
0=ρ
Small instanton singulality
ADHM construction ofNC BPST instantons (N=2,k=1)
ADHM eq. (G=``U(1)’’)
0],[],[],[
21
2211
=+=−++ ∗∗∗∗
IJBBJJIIBBBB ζ
⎟⎠⎞
⎜⎝⎛
=+==ρ
ζρα02( ),0,,2,12,1 JIB
Size slightly fat?position
µνµ FA , : something smooth0→ρ
ASD eq. (G=U(2), C2=-1) Regular! (U(1) instanton!)
0
0
21
2211
=
=+
zz
zzzz
F
FFM
0=ρ
Resolution of the singulality
3. NC Sato’s Theory• Sato’s Theory : one of the most
beautiful theory of solitons– Based on the exsitence of
hierarchies and tau-functions• Sato’s theory reveals essential
aspects of solitons:– Construction of exact solutions– Structure of solution spaces– Infinite conserved quantities– Hidden infinite-dim. symmetry
Is it possible to extend it
to NC spaces ? YES!
NC (KP) Hierarchy:
∗=∂∂ ],[ LBxL
mm
L+∂∂
+∂∂
+∂∂
−
−
−
34
23
12
xm
xm
xm
u
u
u
L+∂
+∂
+∂
−
−
−
34
23
12
)(
)(
)(
xm
xm
xm
uF
uF
uF
Huge amount of ```NC evolution equations’’
0
34
23
12
)(::
≥
−−−
∗∗=+∂+∂+∂+∂=
LLBuuuL
m
xxxx
L
L
),,,( 321 Lxxxuu kk =)(33
2
2323
3
22
2
1
uuuB
uB
B
xx
x
x
′++∂+∂=
+∂=
∂=
Noncommutativity is introduced here
ijji ixx θ=],[
m times
Negative powers of differential operators
jnx
jx
j
nx f
jn
f −∞
=
∂∂⎟⎟⎠
⎞⎜⎜⎝
⎛=∂ ∑ )(:
0o
1)2)(1())1(()2)(1(
L
L
−−−−−−
jjjjnnnn
ffff
fffff
xxx
xxxx
′′+∂′+∂=∂
′′′+∂′′+∂′+∂=∂
2
3322
1233
o
o
Lo
Lo
−∂′′+∂′−∂=∂
−∂′′+∂′−∂=∂−−−−
−−−−
4322
3211
32 xxxx
xxxx
ffff
ffff
)(2
exp)(:)()( xgixfxgxf jiij ⎟
⎠⎞
⎜⎝⎛ ∂∂=∗
rsθ
ijijjiji ixxxxxx θ=∗−∗=∗ :],[
Star product
which makes theories``noncommutative’’:
Closer look at NC (KP) hierarchyFor m=2
2322 2 uuu ′′+′=∂
M
)
)
)
3
2
1
−
−
−
∂
∂
∂
x
x
x
∗+′∗+′′+′=∂ ],[222 32223432 uuuuuuu
∗+′′∗−′∗+′′+′=∂ ],[2242 4222234542 uuuuuuuuu
Infinite kind of fields are representedin terms of one kind of field uu ≡2
MH&K.Toda, [hep-th/0309265]For m=3
M
)1−∂ x 222243223 3333 uuuuuuuu ′∗+∗′+′′+′′+′′′=∂
∗−− ∂+∂+∗+= ],[
43
43)(
43
41 11
yyxyyxxxxxt uuuuuuu
xuux ∂∂
=:
NC KP equation
),,,( 321 Lxxxuu =
x y t∫ ′=∂− x
x xd:1 etc.
(KP hie.) (various hies.)
• KdV hierarchyReduction condition
gives rise to NC KdV hierarchywhich includes NC KdV eq.:
):( 22
2 uBL x +∂==
xxxxt uuuu )(43
41
∗+=
02
=∂∂
lxu
Note
: 2-reduction
: dimensional reduction
l -reduction yields other NC hierarchies which include NC Boussinesq, coupled KdV, Sawada-Kotera, mKdV hierarchies and so on.
NC Burgers hierarchyMH&K.Toda,JPA36(‘03)11981[hepth/0301213]
• NC (1+1)-dim. Burgers equation:
uuuu ′∗+′′= 2& : Non-linear&
Infinite order diff. eq. w.r.t. time !
NC Cole-Hopf transformation
)log( 01 τττ θxu ∂⎯⎯→⎯′∗= →−
ττ ′′=& : Linear &first order diff. eq. w.r.t. time
Integrable !
NC Burgers eq. can be derived from G=U(1) NC ASDYM eq. (One example ofNC Ward’s observation)
4. Conservation Laws
• We have obtained wide class of NC hierarchies and NC (soliton) equations.
• Are they integrable or specialfrom viewpoints of solitontheories? YES !
Now we show the existence of infinite number of conserved quatities which suggests a hiddeninfinite-dimensional symmetry.
Conservation Laws• Conservation laws:
Conservation laws for the hierarchies
iit J∂=∂ σ
σ∫= spacedxQ :
∫∫ ==∂=∂inity
spatiali
ispace tt JdSdxQinf
0σQ
σ : Conserved density
Then is a conserved quantity.
Follwing G.Wilson’s approach, we have:
ijij
xxn
m JBAJLres Ξ∂+∂=+∂=∂ ∗− θ],[1
troublesome
I have succeeded in the evaluation explicitly !
Noncommutativity should be introduced in space-time directions only.
:nr Lres− coefficient of in
rx−∂ nL
Main ResultsInfinite conserved densities for NC hierarchy eqs. (n=1,2,…)
)1(
1
1
11 1
)1( +−−+−−
=
−++
+=
−−+− ◊∂×⎟
⎠⎞
⎜⎝⎛−+= ∑ ∑ −−
− lknmkmiln
m
k
kmn
nl
lknmmin baLresnl
kmθσ
kmx
kkm
mxm
lnx
lln
nx
n
bB
aL
−∞
=−
−∞
=−
∂+∂=
∂+∂=
∑
∑
1
1
◊ : Strachan’s product
mxt ≡
)(21
)!12()1()(:)()(
2
0xg
sxfxgxf
s
jiij
s
s
⎟⎟⎠
⎞⎜⎜⎝
⎛⎟⎠⎞
⎜⎝⎛ ∂∂
+−
=◊ ∑∞
=
rsθ
MH, [hep-th/0311206]
)],([ θixt =Example: NC KP and KdV equations
))()((3 22311 uLresuLresLres nnn ′◊+′◊−= −−− θσ
5. Conclusion and Discussion
• We proved the existence of infinite conserved quantities for wide class of NC hierarchies and gave the infinite conserved densities explicitly.
• Our results strongly suggest that infinite-dim. symmetry would be hidden in NC (soliton) equations.What is it ?
theories of tau-functions are needed(via e.g. Hirota’s bilinearization)the completion of NC Sato’s theory
• The interpretation of space-time noncommutativity should be clarified.
• What is the twistor descriptions ?
There are many things to be seen.
e.g. Kapustin&Kuznetsov&Orlov, Hannabuss,…