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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47018 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{5}\phi_{1}q_{2}^{2}$ | 0.5952 | 0.7742 | 0.7687 | [X:[], M:[0.9324, 1.2029, 1.0676, 0.8043, 0.7971], q:[0.7331, 0.3345], qb:[0.4626, 0.3345], phi:[0.5338]] | [X:[], M:[[-4], [12], [4], [18], [-12]], q:[[-1], [5]], qb:[[-17], [5]], phi:[[2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}q_{2}\tilde{q}_{2}$, ${ }M_{5}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{4}$, ${ }M_{3}$, ${ }\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{5}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }M_{5}^{2}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{4}M_{5}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{5}q_{1}\tilde{q}_{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}^{3}$ | ${}M_{2}M_{5}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{1}$, ${ }M_{5}\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | 1 | t^2.01 + 2*t^2.39 + t^2.41 + 3*t^3.2 + 3*t^3.61 + 2*t^3.99 + t^4.01 + t^4.38 + 2*t^4.4 + t^4.42 + 3*t^4.78 + 2*t^4.8 + t^4.83 + 3*t^5.21 + 5*t^5.59 + 4*t^5.62 + t^6. + 4*t^6.02 + 2*t^6.38 + 5*t^6.41 + t^6.43 + 2*t^6.77 + t^6.79 + 8*t^6.81 + t^6.83 + 3*t^7.17 + 3*t^7.2 + 8*t^7.22 + t^7.24 + t^7.58 + 3*t^7.6 + 4*t^7.62 + 7*t^7.99 + 2*t^8.01 + 5*t^8.03 + 2*t^8.37 - 3*t^8.39 + 4*t^8.41 + 4*t^8.43 + t^8.75 + 2*t^8.78 + 3*t^8.8 + 6*t^8.82 + t^8.84 - t^4.6/y - t^7.01/y + (3*t^7.4)/y + t^7.42/y + t^7.78/y + t^7.8/y + t^8.19/y + (3*t^8.21)/y + (6*t^8.59)/y + (6*t^8.62)/y - t^4.6*y - t^7.01*y + 3*t^7.4*y + t^7.42*y + t^7.78*y + t^7.8*y + t^8.19*y + 3*t^8.21*y + 6*t^8.59*y + 6*t^8.62*y | g1^10*t^2.01 + (2*t^2.39)/g1^12 + g1^18*t^2.41 + 3*g1^4*t^3.2 + 3*g1^12*t^3.61 + (2*t^3.99)/g1^10 + g1^20*t^4.01 + t^4.38/g1^32 + (2*t^4.4)/g1^2 + g1^28*t^4.42 + (3*t^4.78)/g1^24 + 2*g1^6*t^4.8 + g1^36*t^4.83 + 3*g1^14*t^5.21 + (5*t^5.59)/g1^8 + 4*g1^22*t^5.62 + t^6. + 4*g1^30*t^6.02 + (2*t^6.38)/g1^22 + 5*g1^8*t^6.41 + g1^38*t^6.43 + (2*t^6.77)/g1^44 + t^6.79/g1^14 + 8*g1^16*t^6.81 + g1^46*t^6.83 + (3*t^7.17)/g1^36 + (3*t^7.2)/g1^6 + 8*g1^24*t^7.22 + g1^54*t^7.24 + t^7.58/g1^28 + 3*g1^2*t^7.6 + 4*g1^32*t^7.62 + (7*t^7.99)/g1^20 + 2*g1^10*t^8.01 + 5*g1^40*t^8.03 + (2*t^8.37)/g1^42 - (3*t^8.39)/g1^12 + 4*g1^18*t^8.41 + 4*g1^48*t^8.43 + t^8.75/g1^64 + (2*t^8.78)/g1^34 + (3*t^8.8)/g1^4 + 6*g1^26*t^8.82 + g1^56*t^8.84 - (g1^2*t^4.6)/y - (g1^20*t^7.01)/y + (3*t^7.4)/(g1^2*y) + (g1^28*t^7.42)/y + t^7.78/(g1^24*y) + (g1^6*t^7.8)/y + t^8.19/(g1^16*y) + (3*g1^14*t^8.21)/y + (6*t^8.59)/(g1^8*y) + (6*g1^22*t^8.62)/y - g1^2*t^4.6*y - g1^20*t^7.01*y + (3*t^7.4*y)/g1^2 + g1^28*t^7.42*y + (t^7.78*y)/g1^24 + g1^6*t^7.8*y + (t^8.19*y)/g1^16 + 3*g1^14*t^8.21*y + (6*t^8.59*y)/g1^8 + 6*g1^22*t^8.62*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 |
---|---|---|---|---|---|---|---|---|---|
46471 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{2}$ | 0.6244 | 0.811 | 0.77 | [X:[], M:[0.9923, 1.0232, 1.0077, 0.7621, 0.7496], q:[0.7481, 0.2597], qb:[0.4899, 0.4869], phi:[0.5039]] | t^2.24 + 2*t^2.25 + t^2.29 + 2*t^3.02 + 2*t^3.07 + t^3.7 + t^3.76 + t^4.43 + t^4.44 + t^4.45 + t^4.48 + 2*t^4.49 + 3*t^4.5 + 3*t^4.53 + t^4.57 + 2*t^5.26 + 4*t^5.27 + 3*t^5.31 + 3*t^5.32 + 2*t^5.36 + t^5.94 + t^5.95 - 3*t^6. - t^4.51/y - t^4.51*y | detail |