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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59480 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | 1.3956 | 1.6161 | 0.8635 | [X:[], M:[0.8431], q:[0.2732, 0.587], qb:[0.5699, 0.5464], phi:[0.3372]] | [X:[], M:[[-15]], q:[[7], [37]], qb:[[-22], [14]], phi:[[-6]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}$, ${ }q_{2}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}^{5}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{2}q_{1}^{2}q_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{1}^{3}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{1}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$ | ${}\phi_{1}q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ | 0 | t^2.02 + t^2.46 + 2*t^2.53 + t^3.04 + t^3.4 + t^3.47 + t^3.54 + t^4.05 + 2*t^4.41 + 3*t^4.48 + 3*t^4.55 + t^4.92 + 2*t^4.99 + 3*t^5.06 + t^5.35 + 3*t^5.42 + 4*t^5.49 + 3*t^5.56 + t^5.86 + 2*t^5.93 + 3*t^6.07 + t^6.37 + 4*t^6.44 + 4*t^6.51 + 4*t^6.58 + t^6.8 + 2*t^6.87 + 5*t^6.94 + 5*t^7.01 + 5*t^7.08 + 3*t^7.38 + 6*t^7.45 + 7*t^7.52 + 5*t^7.59 + 3*t^7.81 + 7*t^7.88 + 9*t^7.95 + 7*t^8.02 + 6*t^8.09 + t^8.16 + 2*t^8.32 + 2*t^8.39 + 3*t^8.46 + 2*t^8.53 + 5*t^8.6 - t^8.67 + t^8.75 + 6*t^8.82 + 10*t^8.89 + 12*t^8.96 - t^4.01/y - t^5.02/y - t^6.04/y - t^6.47/y - (2*t^6.54)/y - (2*t^7.05)/y - t^7.41/y + (3*t^7.99)/y + t^8.86/y + (2*t^8.93)/y - t^4.01*y - t^5.02*y - t^6.04*y - t^6.47*y - 2*t^6.54*y - 2*t^7.05*y - t^7.41*y + 3*t^7.99*y + t^8.86*y + 2*t^8.93*y | t^2.02/g1^12 + g1^21*t^2.46 + (2*t^2.53)/g1^15 + t^3.04/g1^18 + g1^51*t^3.4 + g1^15*t^3.47 + t^3.54/g1^21 + t^4.05/g1^24 + 2*g1^45*t^4.41 + 3*g1^9*t^4.48 + (3*t^4.55)/g1^27 + g1^42*t^4.92 + 2*g1^6*t^4.99 + (3*t^5.06)/g1^30 + g1^75*t^5.35 + 3*g1^39*t^5.42 + 4*g1^3*t^5.49 + (3*t^5.56)/g1^33 + g1^72*t^5.86 + 2*g1^36*t^5.93 + (3*t^6.07)/g1^36 + g1^69*t^6.37 + 4*g1^33*t^6.44 + (4*t^6.51)/g1^3 + (4*t^6.58)/g1^39 + g1^102*t^6.8 + 2*g1^66*t^6.87 + 5*g1^30*t^6.94 + (5*t^7.01)/g1^6 + (5*t^7.08)/g1^42 + 3*g1^63*t^7.38 + 6*g1^27*t^7.45 + (7*t^7.52)/g1^9 + (5*t^7.59)/g1^45 + 3*g1^96*t^7.81 + 7*g1^60*t^7.88 + 9*g1^24*t^7.95 + (7*t^8.02)/g1^12 + (6*t^8.09)/g1^48 + t^8.16/g1^84 + 2*g1^93*t^8.32 + 2*g1^57*t^8.39 + 3*g1^21*t^8.46 + (2*t^8.53)/g1^15 + (5*t^8.6)/g1^51 - t^8.67/g1^87 + g1^126*t^8.75 + 6*g1^90*t^8.82 + 10*g1^54*t^8.89 + 12*g1^18*t^8.96 - t^4.01/(g1^6*y) - t^5.02/(g1^12*y) - t^6.04/(g1^18*y) - (g1^15*t^6.47)/y - (2*t^6.54)/(g1^21*y) - (2*t^7.05)/(g1^24*y) - (g1^45*t^7.41)/y + (3*g1^6*t^7.99)/y + (g1^72*t^8.86)/y + (2*g1^36*t^8.93)/y - (t^4.01*y)/g1^6 - (t^5.02*y)/g1^12 - (t^6.04*y)/g1^18 - g1^15*t^6.47*y - (2*t^6.54*y)/g1^21 - (2*t^7.05*y)/g1^24 - g1^45*t^7.41*y + 3*g1^6*t^7.99*y + g1^72*t^8.86*y + 2*g1^36*t^8.93*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 |
---|---|---|---|---|---|---|---|---|---|
57732 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ | 1.4351 | 1.6621 | 0.8634 | [X:[], M:[0.8773], q:[0.3567, 0.6022], qb:[0.5205, 0.4151], phi:[0.3509]] | t^2.11 + t^2.32 + 2*t^2.63 + t^3.05 + t^3.16 + t^3.37 + t^3.68 + t^4.1 + t^4.21 + 3*t^4.42 + t^4.63 + 3*t^4.74 + 2*t^4.95 + t^5. + t^5.1 + 2*t^5.16 + 3*t^5.26 + t^5.37 + t^5.42 + 3*t^5.47 + 2*t^5.68 + t^5.74 + 3*t^5.79 - t^6. - t^4.05/y - t^5.11/y - t^4.05*y - t^5.11*y | detail |