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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60948 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$ | 1.3998 | 1.6071 | 0.871 | [X:[1.3651], M:[0.746, 0.746], q:[0.3122, 0.6296], qb:[0.5291, 0.6243], phi:[0.3175]] | [X:[[12]], M:[[-33], [-33]], q:[[13], [7]], qb:[[-10], [26]], phi:[[-6]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{1}$, ${ }M_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }X_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}^{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }M_{2}q_{1}\tilde{q}_{1}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }M_{2}\phi_{1}^{3}$, ${ }q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}q_{1}^{3}$, ${ }\phi_{1}^{2}q_{1}^{2}q_{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{6}$, ${ }M_{2}\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }M_{2}q_{2}\tilde{q}_{1}$ | ${}$ | -2 | 2*t^2.24 + t^2.52 + t^2.81 + t^2.86 + 2*t^3.48 + t^4.1 + 2*t^4.43 + 3*t^4.48 + 3*t^4.71 + 2*t^4.76 + 2*t^5.05 + 2*t^5.1 + t^5.33 + 2*t^5.38 + t^5.62 + 5*t^5.67 + 4*t^5.71 - 2*t^6. + 2*t^6.29 + 4*t^6.33 + 3*t^6.62 + 3*t^6.67 + 4*t^6.71 + t^6.9 + 6*t^6.95 + 3*t^7. + 3*t^7.24 + 5*t^7.29 + 3*t^7.33 + 3*t^7.52 + 6*t^7.57 + 4*t^7.62 + t^7.86 + 10*t^7.9 + 6*t^7.95 + t^8.14 + 9*t^8.19 - 3*t^8.24 + t^8.43 + 6*t^8.48 + 3*t^8.52 + 7*t^8.57 - 4*t^8.81 + 5*t^8.86 + 4*t^8.9 + 5*t^8.95 + t^8.86/y^2 - t^3.95/y - t^4.9/y - (2*t^6.19)/y - t^6.48/y - t^6.76/y - t^6.81/y - (2*t^7.14)/y - (2*t^7.43)/y + t^7.48/y + t^7.76/y + (2*t^8.05)/y + (2*t^8.1)/y + t^8.33/y - t^8.38/y - (3*t^8.43)/y + t^8.67/y + (2*t^8.71)/y - t^3.95*y - t^4.9*y - 2*t^6.19*y - t^6.48*y - t^6.76*y - t^6.81*y - 2*t^7.14*y - 2*t^7.43*y + t^7.48*y + t^7.76*y + 2*t^8.05*y + 2*t^8.1*y + t^8.33*y - t^8.38*y - 3*t^8.43*y + t^8.67*y + 2*t^8.71*y + t^8.86*y^2 | (2*t^2.24)/g1^33 + g1^3*t^2.52 + g1^39*t^2.81 + t^2.86/g1^18 + (2*t^3.48)/g1^3 + g1^12*t^4.1 + (2*t^4.43)/g1^9 + (3*t^4.48)/g1^66 + 3*g1^27*t^4.71 + (2*t^4.76)/g1^30 + 2*g1^6*t^5.05 + (2*t^5.1)/g1^51 + g1^42*t^5.33 + (2*t^5.38)/g1^15 + g1^78*t^5.62 + 5*g1^21*t^5.67 + (4*t^5.71)/g1^36 - 2*t^6. + 2*g1^36*t^6.29 + (4*t^6.33)/g1^21 + 3*g1^15*t^6.62 + (3*t^6.67)/g1^42 + (4*t^6.71)/g1^99 + g1^51*t^6.9 + (6*t^6.95)/g1^6 + (3*t^7.)/g1^63 + 3*g1^30*t^7.24 + (5*t^7.29)/g1^27 + (3*t^7.33)/g1^84 + 3*g1^66*t^7.52 + 6*g1^9*t^7.57 + (4*t^7.62)/g1^48 + g1^45*t^7.86 + (10*t^7.9)/g1^12 + (6*t^7.95)/g1^69 + g1^81*t^8.14 + 9*g1^24*t^8.19 - (3*t^8.24)/g1^33 + g1^117*t^8.43 + 6*g1^60*t^8.48 + 3*g1^3*t^8.52 + (7*t^8.57)/g1^54 - 4*g1^39*t^8.81 + (5*t^8.86)/g1^18 + (4*t^8.9)/g1^75 + (5*t^8.95)/g1^132 + t^8.86/(g1^18*y^2) - t^3.95/(g1^6*y) - t^4.9/(g1^12*y) - (2*t^6.19)/(g1^39*y) - t^6.48/(g1^3*y) - (g1^33*t^6.76)/y - t^6.81/(g1^24*y) - (2*t^7.14)/(g1^45*y) - (2*t^7.43)/(g1^9*y) + t^7.48/(g1^66*y) + t^7.76/(g1^30*y) + (2*g1^6*t^8.05)/y + (2*t^8.1)/(g1^51*y) + (g1^42*t^8.33)/y - t^8.38/(g1^15*y) - (3*t^8.43)/(g1^72*y) + (g1^21*t^8.67)/y + (2*t^8.71)/(g1^36*y) - (t^3.95*y)/g1^6 - (t^4.9*y)/g1^12 - (2*t^6.19*y)/g1^39 - (t^6.48*y)/g1^3 - g1^33*t^6.76*y - (t^6.81*y)/g1^24 - (2*t^7.14*y)/g1^45 - (2*t^7.43*y)/g1^9 + (t^7.48*y)/g1^66 + (t^7.76*y)/g1^30 + 2*g1^6*t^8.05*y + (2*t^8.1*y)/g1^51 + g1^42*t^8.33*y - (t^8.38*y)/g1^15 - (3*t^8.43*y)/g1^72 + g1^21*t^8.67*y + (2*t^8.71*y)/g1^36 + (t^8.86*y^2)/g1^18 |
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 |
---|---|---|---|---|---|---|---|---|---|
58721 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ | 1.4205 | 1.6281 | 0.8725 | [X:[1.3591], M:[0.7624, 0.7624], q:[0.3717, 0.6921], qb:[0.4681, 0.5455], phi:[0.3204]] | 2*t^2.29 + t^2.52 + t^2.75 + t^2.88 + 2*t^3.48 + t^4.08 + 2*t^4.44 + 3*t^4.57 + 2*t^4.67 + 2*t^4.81 + 2*t^5.04 + 2*t^5.17 + 2*t^5.27 + 2*t^5.4 + t^5.41 + t^5.5 + 3*t^5.64 + 4*t^5.77 - 3*t^6. - t^3.96/y - t^4.92/y - t^3.96*y - t^4.92*y | detail |