Chosen Fixed Point
Here is the data for the chosen fixed point.
$F_{UV}$ represents the flavor symmetries in the UV Lagrangian, and $F_{IR}$ represents the flavor symmetries in the IR. $F_{UV}$ and $F_{IR}$ can differ due to accidental symmetry enhancement.
The number of marginal operators, $n_{marginal}$, minus the dimension of flavor symmetries in IR, $|F_{IR}|$, corresponds to the coefficient of $t^6$ in the superconformal index.
# | Theory | Superpotential | Central charge $a$ | Central charge $c$ | Ratio $a/c$ | Matter field: $R$-charge | U(1) part of $F_{UV}$ | Rank of $F_{UV}$ | Rational |
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56351 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{3}M_{4}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{6}$ + ${ }M_{7}\phi_{1}q_{2}^{2}$ | 0.6538 | 0.8125 | 0.8047 | [M:[1.0577, 0.7113, 0.8268, 1.1732, 1.067, 1.2887, 0.6928], q:[0.5242, 0.418], qb:[0.7644, 0.4088], phi:[0.4711]] | [M:[[4], [-20], [-12], [12], [-30], [20], [48]], q:[[19], [-23]], qb:[[1], [11]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}M_{7}$, ${ }M_{3}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }M_{5}$, ${ }M_{4}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{6}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{7}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{3}M_{7}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{7}$, ${ }M_{5}M_{7}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{4}M_{7}$, ${ }M_{7}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{3}$, ${ }\phi_{1}^{4}$, ${ }M_{6}M_{7}$, ${ }M_{7}\phi_{1}\tilde{q}_{2}^{2}$ | ${}$ | -1 | t^2.078 + t^2.48 + t^2.827 + t^3.173 + t^3.201 + t^3.52 + t^3.547 + 2*t^3.866 + t^3.894 + t^4.157 + t^4.212 + t^4.24 + 2*t^4.559 + t^4.905 + t^4.961 + t^5.252 + t^5.279 + t^5.307 + t^5.598 + t^5.626 + t^5.654 + 2*t^5.944 - t^6. + t^6.028 + t^6.235 + t^6.291 + t^6.346 + 2*t^6.374 + t^6.402 + 2*t^6.637 + 2*t^6.693 + 2*t^6.721 + t^6.748 + t^6.983 + 3*t^7.039 + 2*t^7.067 + t^7.33 + t^7.358 + 3*t^7.386 + t^7.413 + t^7.441 + t^7.676 + t^7.704 + 3*t^7.732 + 2*t^7.76 + t^7.788 + 2*t^8.023 + t^8.078 + 2*t^8.106 + t^8.313 + t^8.369 + 3*t^8.425 + t^8.453 + 2*t^8.715 + 3*t^8.771 + t^8.799 - t^8.827 + t^8.855 - t^4.413/y - t^6.492/y + t^7.212/y + t^7.559/y - t^7.614/y + t^7.905/y + t^8.252/y + t^8.279/y + t^8.307/y + t^8.335/y - t^8.57/y + t^8.598/y + t^8.626/y + t^8.654/y + t^8.681/y + (2*t^8.944)/y + t^8.972/y - t^4.413*y - t^6.492*y + t^7.212*y + t^7.559*y - t^7.614*y + t^7.905*y + t^8.252*y + t^8.279*y + t^8.307*y + t^8.335*y - t^8.57*y + t^8.598*y + t^8.626*y + t^8.654*y + t^8.681*y + 2*t^8.944*y + t^8.972*y | g1^48*t^2.078 + t^2.48/g1^12 + t^2.827/g1^4 + g1^4*t^3.173 + t^3.201/g1^30 + g1^12*t^3.52 + t^3.547/g1^22 + 2*g1^20*t^3.866 + t^3.894/g1^14 + g1^96*t^4.157 + g1^28*t^4.212 + t^4.24/g1^6 + 2*g1^36*t^4.559 + g1^44*t^4.905 + t^4.961/g1^24 + g1^52*t^5.252 + g1^18*t^5.279 + t^5.307/g1^16 + g1^60*t^5.598 + g1^26*t^5.626 + t^5.654/g1^8 + 2*g1^68*t^5.944 - t^6. + t^6.028/g1^34 + g1^144*t^6.235 + g1^76*t^6.291 + g1^8*t^6.346 + (2*t^6.374)/g1^26 + t^6.402/g1^60 + 2*g1^84*t^6.637 + 2*g1^16*t^6.693 + (2*t^6.721)/g1^18 + t^6.748/g1^52 + g1^92*t^6.983 + 3*g1^24*t^7.039 + (2*t^7.067)/g1^10 + g1^100*t^7.33 + g1^66*t^7.358 + 3*g1^32*t^7.386 + t^7.413/g1^2 + t^7.441/g1^36 + g1^108*t^7.676 + g1^74*t^7.704 + 3*g1^40*t^7.732 + 2*g1^6*t^7.76 + t^7.788/g1^28 + 2*g1^116*t^8.023 + g1^48*t^8.078 + 2*g1^14*t^8.106 + g1^192*t^8.313 + g1^124*t^8.369 + 3*g1^56*t^8.425 + g1^22*t^8.453 + 2*g1^132*t^8.715 + 3*g1^64*t^8.771 + g1^30*t^8.799 - t^8.827/g1^4 + t^8.855/g1^38 - t^4.413/(g1^2*y) - (g1^46*t^6.492)/y + (g1^28*t^7.212)/y + (g1^36*t^7.559)/y - t^7.614/(g1^32*y) + (g1^44*t^7.905)/y + (g1^52*t^8.252)/y + (g1^18*t^8.279)/y + t^8.307/(g1^16*y) + t^8.335/(g1^50*y) - (g1^94*t^8.57)/y + (g1^60*t^8.598)/y + (g1^26*t^8.626)/y + t^8.654/(g1^8*y) + t^8.681/(g1^42*y) + (2*g1^68*t^8.944)/y + (g1^34*t^8.972)/y - (t^4.413*y)/g1^2 - g1^46*t^6.492*y + g1^28*t^7.212*y + g1^36*t^7.559*y - (t^7.614*y)/g1^32 + g1^44*t^7.905*y + g1^52*t^8.252*y + g1^18*t^8.279*y + (t^8.307*y)/g1^16 + (t^8.335*y)/g1^50 - g1^94*t^8.57*y + g1^60*t^8.598*y + g1^26*t^8.626*y + (t^8.654*y)/g1^8 + (t^8.681*y)/g1^42 + 2*g1^68*t^8.944*y + g1^34*t^8.972*y |
Deformation
Here is the data for the deformed fixed points from the chosen fixed point.
# | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from Other Seed Theories
Here is a list of equivalent fixed points from other gauge theories.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from the Same Seed Theory
Below is a list of equivalent fixed points from the same seed theories.
id | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | More Info. | Rational |
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Previous Theory
The previous fixed point before deforming to get the chosen fixed point.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
---|---|---|---|---|---|---|---|---|---|
52084 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{3}M_{4}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{6}$ | 0.6333 | 0.7731 | 0.8192 | [M:[1.0593, 0.7037, 0.8222, 1.1778, 1.0556, 1.2963], q:[0.5315, 0.4093], qb:[0.7648, 0.4129], phi:[0.4704]] | t^2.467 + t^2.822 + t^3.167 + t^3.178 + t^3.522 + t^3.533 + t^3.867 + t^3.878 + 2*t^3.889 + t^4.233 + t^4.244 + t^4.6 + t^4.933 + t^5.289 + t^5.644 + t^5.989 - t^6. - t^4.411/y - t^4.411*y | detail |