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 |
---|---|---|---|---|---|---|---|---|---|
46078 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ | 0.6066 | 0.7783 | 0.7794 | [X:[], M:[0.9857, 0.7607, 1.043], q:[0.7464, 0.2679], qb:[0.4642, 0.4928], phi:[0.5072]] | [X:[], M:[[4], [-3], [-12]], q:[[1], [-5]], qb:[[10], [2]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}q_{2}\tilde{q}_{1}$, ${ }M_{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{1}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }\phi_{1}q_{2}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{1}M_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ }M_{1}^{2}$, ${ }M_{2}q_{1}\tilde{q}_{1}$ | ${}M_{2}q_{1}\tilde{q}_{2}$ | 0 | t^2.2 + 2*t^2.28 + t^2.96 + t^3.04 + 2*t^3.13 + t^3.63 + t^3.72 + t^3.8 + t^4.31 + 2*t^4.39 + 3*t^4.48 + 3*t^4.56 + t^5.15 + 3*t^5.24 + 3*t^5.33 + 3*t^5.41 + t^5.83 + 2*t^5.91 + 2*t^6.09 + 2*t^6.17 + 3*t^6.26 + t^6.5 + 3*t^6.59 + 3*t^6.67 + 5*t^6.76 + 4*t^6.85 + t^6.93 + t^7.26 + 2*t^7.35 + 3*t^7.44 + 5*t^7.52 + 5*t^7.61 + 4*t^7.69 + t^7.94 + 2*t^8.02 + t^8.11 - t^8.28 + 3*t^8.37 + 4*t^8.45 + 4*t^8.54 + t^8.61 + 2*t^8.7 + 4*t^8.79 + 4*t^8.87 + t^8.96 - t^4.52/y - t^6.8/y + t^7.39/y + (2*t^7.48)/y + t^7.56/y - t^7.65/y + t^8.15/y + (4*t^8.24)/y + (4*t^8.33)/y + (4*t^8.41)/y + t^8.83/y + (3*t^8.91)/y - t^4.52*y - t^6.8*y + t^7.39*y + 2*t^7.48*y + t^7.56*y - t^7.65*y + t^8.15*y + 4*t^8.24*y + 4*t^8.33*y + 4*t^8.41*y + t^8.83*y + 3*t^8.91*y | g1^5*t^2.2 + (2*t^2.28)/g1^3 + g1^4*t^2.96 + t^3.04/g1^4 + (2*t^3.13)/g1^12 + g1^11*t^3.63 + g1^3*t^3.72 + t^3.8/g1^5 + g1^18*t^4.31 + 2*g1^10*t^4.39 + 3*g1^2*t^4.48 + (3*t^4.56)/g1^6 + g1^9*t^5.15 + 3*g1*t^5.24 + (3*t^5.33)/g1^7 + (3*t^5.41)/g1^15 + g1^16*t^5.83 + 2*g1^8*t^5.91 + (2*t^6.09)/g1^8 + (2*t^6.17)/g1^16 + (3*t^6.26)/g1^24 + g1^23*t^6.5 + 3*g1^15*t^6.59 + 3*g1^7*t^6.67 + (5*t^6.76)/g1 + (4*t^6.85)/g1^9 + t^6.93/g1^17 + g1^22*t^7.26 + 2*g1^14*t^7.35 + 3*g1^6*t^7.44 + (5*t^7.52)/g1^2 + (5*t^7.61)/g1^10 + (4*t^7.69)/g1^18 + g1^29*t^7.94 + 2*g1^21*t^8.02 + g1^13*t^8.11 - t^8.28/g1^3 + (3*t^8.37)/g1^11 + (4*t^8.45)/g1^19 + (4*t^8.54)/g1^27 + g1^36*t^8.61 + 2*g1^28*t^8.7 + 4*g1^20*t^8.79 + 4*g1^12*t^8.87 + g1^4*t^8.96 - t^4.52/(g1^2*y) - t^6.8/(g1^5*y) + (g1^10*t^7.39)/y + (2*g1^2*t^7.48)/y + t^7.56/(g1^6*y) - t^7.65/(g1^14*y) + (g1^9*t^8.15)/y + (4*g1*t^8.24)/y + (4*t^8.33)/(g1^7*y) + (4*t^8.41)/(g1^15*y) + (g1^16*t^8.83)/y + (3*g1^8*t^8.91)/y - (t^4.52*y)/g1^2 - (t^6.8*y)/g1^5 + g1^10*t^7.39*y + 2*g1^2*t^7.48*y + (t^7.56*y)/g1^6 - (t^7.65*y)/g1^14 + g1^9*t^8.15*y + 4*g1*t^8.24*y + (4*t^8.33*y)/g1^7 + (4*t^8.41*y)/g1^15 + g1^16*t^8.83*y + 3*g1^8*t^8.91*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 |
---|---|---|---|---|---|---|---|---|
46651 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{4}$ | 0.6055 | 0.7768 | 0.7796 | [X:[], M:[0.9916, 0.7563, 1.0252, 1.0084], q:[0.7479, 0.2605], qb:[0.479, 0.4958], phi:[0.5042]] | t^2.22 + 2*t^2.27 + 2*t^3.03 + 2*t^3.08 + t^3.68 + t^3.73 + t^3.78 + t^4.39 + 2*t^4.44 + 3*t^4.49 + 3*t^4.54 + 2*t^5.24 + 5*t^5.29 + 3*t^5.34 + t^5.9 + t^5.95 - t^6. - t^4.51/y - t^4.51*y | detail | |
46455 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ | 0.6244 | 0.8107 | 0.7701 | [X:[], M:[0.994, 0.7545, 1.0181, 0.7666], q:[0.7485, 0.2575], qb:[0.4849, 0.497], phi:[0.503]] | t^2.23 + 2*t^2.26 + t^2.3 + t^2.98 + t^3.02 + 2*t^3.05 + t^3.74 + t^3.77 + t^4.42 + 2*t^4.45 + 3*t^4.49 + 4*t^4.53 + 2*t^4.56 + t^4.6 + t^5.21 + 3*t^5.25 + 4*t^5.28 + 4*t^5.32 + 2*t^5.35 - t^4.51/y - t^4.51*y | detail |
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 |
---|---|---|---|---|---|---|---|---|---|
45945 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$ | 0.6129 | 0.79 | 0.7758 | [X:[], M:[0.9693, 0.773], q:[0.7423, 0.2884], qb:[0.4233, 0.4847], phi:[0.5153]] | t^2.13 + 2*t^2.32 + t^2.72 + t^2.91 + t^3.09 + t^3.28 + t^3.5 + t^3.68 + t^3.87 + t^4.09 + 2*t^4.27 + 3*t^4.45 + 3*t^4.64 + t^4.86 + 3*t^5.04 + 3*t^5.23 + 2*t^5.41 + t^5.45 + t^5.6 + 2*t^5.63 + 3*t^5.82 + t^6. - t^4.55/y - t^4.55*y | detail |