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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56637 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }M_{6}q_{2}\tilde{q}_{2}$ + ${ }M_{7}q_{1}\tilde{q}_{2}$ | 0.6628 | 0.8259 | 0.8025 | [M:[1.1264, 0.7356, 0.8736, 0.8736, 1.2184, 0.8276, 0.6897], q:[0.5057, 0.3678], qb:[0.7586, 0.8046], phi:[0.3908]] | [M:[[-16], [-14], [16], [16], [4], [6], [-24]], q:[[23], [-7]], qb:[[-9], [1]], phi:[[-2]]] | 1 | {a: 26755/40368, c: 16669/20184, M1: 98/87, M2: 64/87, M3: 76/87, M4: 76/87, M5: 106/87, M6: 24/29, M7: 20/29, q1: 44/87, q2: 32/87, qb1: 22/29, qb2: 70/87, phi1: 34/87} |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{7}$, ${ }M_{2}$, ${ }M_{6}$, ${ }M_{3}$, ${ }M_{4}$, ${ }M_{1}$, ${ }M_{5}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{7}^{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{2}M_{7}$, ${ }M_{2}^{2}$, ${ }M_{6}M_{7}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{2}M_{6}$, ${ }M_{3}M_{7}$, ${ }M_{4}M_{7}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{4}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{3}M_{6}$, ${ }M_{4}M_{6}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}^{2}$, ${ }M_{1}M_{7}$, ${ }M_{5}M_{7}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{1}M_{6}$, ${ }M_{7}\phi_{1}q_{1}q_{2}$ | ${}$ | -1 | t^2.069 + t^2.207 + t^2.483 + 2*t^2.621 + t^3.379 + t^3.655 + t^3.793 + t^4.138 + t^4.207 + t^4.276 + t^4.414 + 2*t^4.552 + 4*t^4.69 + t^4.828 + 2*t^4.966 + 2*t^5.103 + 2*t^5.241 + t^5.448 + 2*t^5.724 + 2*t^5.862 - t^6. + t^6.207 + 3*t^6.276 + t^6.345 + t^6.414 + t^6.483 + 3*t^6.621 + t^6.69 + 4*t^6.759 + 2*t^6.828 + 2*t^6.897 + 3*t^7.034 + 4*t^7.172 + 3*t^7.31 + 3*t^7.448 + t^7.517 + 3*t^7.586 + t^7.724 + 2*t^7.793 + 2*t^7.862 + 3*t^7.931 + t^8. - t^8.069 - 2*t^8.207 + t^8.276 + 4*t^8.345 + 2*t^8.414 - 2*t^8.483 + t^8.552 - 4*t^8.621 + 3*t^8.69 + 2*t^8.759 + 5*t^8.828 + 3*t^8.897 + 2*t^8.966 - t^4.172/y - t^6.241/y - t^6.379/y - t^6.655/y - t^6.793/y + t^7.276/y + (2*t^7.552)/y + (4*t^7.69)/y + (2*t^7.828)/y + t^7.966/y + (3*t^8.103)/y + t^8.241/y - t^8.31/y + t^8.862/y - t^4.172*y - t^6.241*y - t^6.379*y - t^6.655*y - t^6.793*y + t^7.276*y + 2*t^7.552*y + 4*t^7.69*y + 2*t^7.828*y + t^7.966*y + 3*t^8.103*y + t^8.241*y - t^8.31*y + t^8.862*y | t^2.069/g1^24 + t^2.207/g1^14 + g1^6*t^2.483 + 2*g1^16*t^2.621 + t^3.379/g1^16 + g1^4*t^3.655 + g1^14*t^3.793 + t^4.138/g1^48 + g1^44*t^4.207 + t^4.276/g1^38 + t^4.414/g1^28 + (2*t^4.552)/g1^18 + (4*t^4.69)/g1^8 + g1^2*t^4.828 + 2*g1^12*t^4.966 + 2*g1^22*t^5.103 + 2*g1^32*t^5.241 + t^5.448/g1^40 + (2*t^5.724)/g1^20 + (2*t^5.862)/g1^10 - t^6. + t^6.207/g1^72 + 3*g1^20*t^6.276 + t^6.345/g1^62 + g1^30*t^6.414 + t^6.483/g1^52 + (3*t^6.621)/g1^42 + g1^50*t^6.69 + (4*t^6.759)/g1^32 + 2*g1^60*t^6.828 + (2*t^6.897)/g1^22 + (3*t^7.034)/g1^12 + (4*t^7.172)/g1^2 + 3*g1^8*t^7.31 + 3*g1^18*t^7.448 + t^7.517/g1^64 + 3*g1^28*t^7.586 + g1^38*t^7.724 + (2*t^7.793)/g1^44 + 2*g1^48*t^7.862 + (3*t^7.931)/g1^34 + g1^58*t^8. - t^8.069/g1^24 - (2*t^8.207)/g1^14 + t^8.276/g1^96 + (4*t^8.345)/g1^4 + t^8.414/g1^86 + g1^88*t^8.414 - 2*g1^6*t^8.483 + t^8.552/g1^76 - 4*g1^16*t^8.621 + (3*t^8.69)/g1^66 + 2*g1^26*t^8.759 + (5*t^8.828)/g1^56 + 3*g1^36*t^8.897 + (2*t^8.966)/g1^46 - t^4.172/(g1^2*y) - t^6.241/(g1^26*y) - t^6.379/(g1^16*y) - (g1^4*t^6.655)/y - (g1^14*t^6.793)/y + t^7.276/(g1^38*y) + (2*t^7.552)/(g1^18*y) + (4*t^7.69)/(g1^8*y) + (2*g1^2*t^7.828)/y + (g1^12*t^7.966)/y + (3*g1^22*t^8.103)/y + (g1^32*t^8.241)/y - t^8.31/(g1^50*y) + t^8.862/(g1^10*y) - (t^4.172*y)/g1^2 - (t^6.241*y)/g1^26 - (t^6.379*y)/g1^16 - g1^4*t^6.655*y - g1^14*t^6.793*y + (t^7.276*y)/g1^38 + (2*t^7.552*y)/g1^18 + (4*t^7.69*y)/g1^8 + 2*g1^2*t^7.828*y + g1^12*t^7.966*y + 3*g1^22*t^8.103*y + g1^32*t^8.241*y - (t^8.31*y)/g1^50 + (t^8.862*y)/g1^10 |
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 |
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54978 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }M_{6}q_{2}\tilde{q}_{2}$ | 0.6421 | 0.7861 | 0.8168 | [M:[1.1304, 0.7391, 0.8696, 0.8696, 1.2174, 0.8261], q:[0.5001, 0.3695], qb:[0.7608, 0.8044], phi:[0.3913]] | t^2.217 + t^2.478 + 2*t^2.609 + t^3.391 + t^3.652 + t^3.783 + t^3.913 + t^4.174 + t^4.434 + t^4.565 + 2*t^4.696 + t^4.826 + 2*t^4.957 + 2*t^5.087 + 2*t^5.218 + t^5.739 + t^5.869 - t^6. - t^4.174/y - t^4.174*y | detail |