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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48258 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}\phi_{1}q_{2}^{2}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{1}M_{5}$ | 0.6334 | 0.8272 | 0.7657 | [M:[0.9496, 0.8278, 0.8487, 0.8487, 1.0504], q:[0.7374, 0.313], qb:[0.4348, 0.4139], phi:[0.5252]] | [M:[[-4], [26], [-12], [-12], [4]], q:[[-1], [5]], qb:[[-25], [13]], phi:[[2]]] |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}q_{2}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{2}$, ${ }M_{3}$, ${ }M_{4}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}$, ${ }\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{5}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{2}M_{5}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{4}M_{5}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$ | ${}\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ | -2 | t^2.181 + t^2.243 + t^2.484 + 3*t^2.546 + 2*t^3.151 + t^3.757 + t^3.819 + t^4.059 + t^4.122 + t^4.184 + t^4.362 + t^4.424 + t^4.487 + t^4.664 + 4*t^4.727 + 3*t^4.79 + t^4.967 + 3*t^5.03 + 6*t^5.092 + 2*t^5.332 + 2*t^5.395 + t^5.635 + 4*t^5.697 - 2*t^6. + 2*t^6.24 + 5*t^6.303 + 3*t^6.365 + t^6.428 + 2*t^6.543 + 3*t^6.605 + 3*t^6.668 + 4*t^6.73 + t^6.845 + 3*t^6.908 + 3*t^6.97 + 2*t^7.033 + t^7.148 + 4*t^7.21 + 7*t^7.273 + 7*t^7.336 + t^7.451 + 4*t^7.513 + 4*t^7.576 + 10*t^7.638 + 2*t^7.816 + 4*t^7.878 + 3*t^7.941 + t^8.003 + 2*t^8.118 - t^8.181 + 4*t^8.243 + t^8.306 + t^8.369 + t^8.421 - t^8.484 - 6*t^8.546 + t^8.671 + 3*t^8.724 + 5*t^8.786 + 6*t^8.849 + 6*t^8.911 + 4*t^8.974 - t^4.576/y - t^7.059/y - (2*t^7.122)/y + (2*t^7.424)/y + t^7.664/y + (3*t^7.727)/y + (3*t^7.79)/y + (5*t^8.03)/y + (4*t^8.092)/y + (2*t^8.332)/y + (2*t^8.395)/y + (2*t^8.635)/y + (6*t^8.697)/y + t^8.937/y - t^4.576*y - t^7.059*y - 2*t^7.122*y + 2*t^7.424*y + t^7.664*y + 3*t^7.727*y + 3*t^7.79*y + 5*t^8.03*y + 4*t^8.092*y + 2*t^8.332*y + 2*t^8.395*y + 2*t^8.635*y + 6*t^8.697*y + t^8.937*y | g1^18*t^2.181 + t^2.243/g1^20 + g1^26*t^2.484 + (3*t^2.546)/g1^12 + 2*g1^4*t^3.151 + g1^20*t^3.757 + t^3.819/g1^18 + g1^28*t^4.059 + t^4.122/g1^10 + t^4.184/g1^48 + g1^36*t^4.362 + t^4.424/g1^2 + t^4.487/g1^40 + g1^44*t^4.664 + 4*g1^6*t^4.727 + (3*t^4.79)/g1^32 + g1^52*t^4.967 + 3*g1^14*t^5.03 + (6*t^5.092)/g1^24 + 2*g1^22*t^5.332 + (2*t^5.395)/g1^16 + g1^30*t^5.635 + (4*t^5.697)/g1^8 - 2*t^6. + 2*g1^46*t^6.24 + 5*g1^8*t^6.303 + (3*t^6.365)/g1^30 + t^6.428/g1^68 + 2*g1^54*t^6.543 + 3*g1^16*t^6.605 + (3*t^6.668)/g1^22 + (4*t^6.73)/g1^60 + g1^62*t^6.845 + 3*g1^24*t^6.908 + (3*t^6.97)/g1^14 + (2*t^7.033)/g1^52 + g1^70*t^7.148 + 4*g1^32*t^7.21 + (7*t^7.273)/g1^6 + (7*t^7.336)/g1^44 + g1^78*t^7.451 + 4*g1^40*t^7.513 + 4*g1^2*t^7.576 + (10*t^7.638)/g1^36 + 2*g1^48*t^7.816 + 4*g1^10*t^7.878 + (3*t^7.941)/g1^28 + t^8.003/g1^66 + 2*g1^56*t^8.118 - g1^18*t^8.181 + (4*t^8.243)/g1^20 + t^8.306/g1^58 + t^8.369/g1^96 + g1^64*t^8.421 - g1^26*t^8.484 - (6*t^8.546)/g1^12 + t^8.671/g1^88 + 3*g1^72*t^8.724 + 5*g1^34*t^8.786 + (6*t^8.849)/g1^4 + (6*t^8.911)/g1^42 + (4*t^8.974)/g1^80 - (g1^2*t^4.576)/y - (g1^28*t^7.059)/y - (2*t^7.122)/(g1^10*y) + (2*t^7.424)/(g1^2*y) + (g1^44*t^7.664)/y + (3*g1^6*t^7.727)/y + (3*t^7.79)/(g1^32*y) + (5*g1^14*t^8.03)/y + (4*t^8.092)/(g1^24*y) + (2*g1^22*t^8.332)/y + (2*t^8.395)/(g1^16*y) + (2*g1^30*t^8.635)/y + (6*t^8.697)/(g1^8*y) + (g1^38*t^8.937)/y - g1^2*t^4.576*y - g1^28*t^7.059*y - (2*t^7.122*y)/g1^10 + (2*t^7.424*y)/g1^2 + g1^44*t^7.664*y + 3*g1^6*t^7.727*y + (3*t^7.79*y)/g1^32 + 5*g1^14*t^8.03*y + (4*t^8.092*y)/g1^24 + 2*g1^22*t^8.332*y + (2*t^8.395*y)/g1^16 + 2*g1^30*t^8.635*y + (6*t^8.697*y)/g1^8 + g1^38*t^8.937*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 |
---|---|---|---|---|---|---|---|---|---|
46507 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}\phi_{1}q_{2}^{2}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ | 0.6381 | 0.8353 | 0.764 | [M:[0.9488, 0.8329, 0.8463, 0.8463], q:[0.7372, 0.314], qb:[0.4299, 0.4165], phi:[0.5256]] | t^2.191 + t^2.232 + t^2.499 + 3*t^2.539 + t^2.846 + t^3.154 + t^3.768 + t^3.809 + t^4.076 + t^4.116 + t^4.156 + t^4.383 + t^4.423 + t^4.463 + t^4.69 + 4*t^4.73 + 3*t^4.771 + t^4.998 + 4*t^5.038 + 7*t^5.078 + 2*t^5.345 + 4*t^5.385 + 2*t^5.693 - t^6. - t^4.577/y - t^4.577*y | detail |