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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56572 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{6}\phi_{1}^{2}$ + ${ }M_{1}M_{2}$ + ${ }M_{3}M_{5}$ + ${ }M_{6}M_{7}$ | 0.6959 | 0.8548 | 0.8141 | [M:[0.9528, 1.0472, 1.0283, 0.9339, 0.9717, 1.0094, 0.9906], q:[0.5047, 0.5425], qb:[0.4481, 0.5236], phi:[0.4953]] | [M:[[-10], [10], [6], [-14], [-6], [2], [-2]], q:[[1], [9]], qb:[[-11], [5]], phi:[[-1]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{4}$, ${ }M_{1}$, ${ }M_{5}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{1}M_{5}$, ${ }M_{4}M_{7}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{5}^{2}$, ${ }M_{1}M_{7}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{5}M_{7}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{2}M_{4}$, ${ }M_{7}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$ | ${}$ | -2 | t^2.802 + t^2.858 + t^2.915 + 2*t^2.972 + t^3.085 + t^3.142 + t^4.174 + t^4.344 + t^4.401 + t^4.457 + t^4.514 + t^4.571 + 2*t^4.628 + t^4.684 + t^4.741 + t^5.603 + t^5.66 + t^5.717 + 2*t^5.773 + 2*t^5.83 + 2*t^5.887 + 3*t^5.943 - 2*t^6. + t^6.113 + t^6.976 + t^7.032 + t^7.089 + 3*t^7.146 + 2*t^7.259 + 4*t^7.316 + 2*t^7.372 + 3*t^7.429 + 2*t^7.486 + 2*t^7.543 + 4*t^7.599 + t^7.656 + 2*t^7.713 + t^7.826 + t^7.883 + t^8.348 + t^8.405 + t^8.462 + 2*t^8.518 + 3*t^8.575 + 2*t^8.632 + 2*t^8.688 + 4*t^8.745 + 2*t^8.802 + t^8.915 - 5*t^8.972 - t^4.486/y - t^7.287/y - t^7.457/y + t^7.514/y + t^7.684/y + t^8.66/y + t^8.717/y + (3*t^8.773)/y + (2*t^8.83)/y + (3*t^8.887)/y + (3*t^8.943)/y - t^4.486*y - t^7.287*y - t^7.457*y + t^7.514*y + t^7.684*y + t^8.66*y + t^8.717*y + 3*t^8.773*y + 2*t^8.83*y + 3*t^8.887*y + 3*t^8.943*y | t^2.802/g1^14 + t^2.858/g1^10 + t^2.915/g1^6 + (2*t^2.972)/g1^2 + g1^6*t^3.085 + g1^10*t^3.142 + t^4.174/g1^23 + t^4.344/g1^11 + t^4.401/g1^7 + t^4.457/g1^3 + g1*t^4.514 + g1^5*t^4.571 + 2*g1^9*t^4.628 + g1^13*t^4.684 + g1^17*t^4.741 + t^5.603/g1^28 + t^5.66/g1^24 + t^5.717/g1^20 + (2*t^5.773)/g1^16 + (2*t^5.83)/g1^12 + (2*t^5.887)/g1^8 + (3*t^5.943)/g1^4 - 2*t^6. + g1^8*t^6.113 + t^6.976/g1^37 + t^7.032/g1^33 + t^7.089/g1^29 + (3*t^7.146)/g1^25 + (2*t^7.259)/g1^17 + (4*t^7.316)/g1^13 + (2*t^7.372)/g1^9 + (3*t^7.429)/g1^5 + (2*t^7.486)/g1 + 2*g1^3*t^7.543 + 4*g1^7*t^7.599 + g1^11*t^7.656 + 2*g1^15*t^7.713 + g1^23*t^7.826 + g1^27*t^7.883 + t^8.348/g1^46 + t^8.405/g1^42 + t^8.462/g1^38 + (2*t^8.518)/g1^34 + (3*t^8.575)/g1^30 + (2*t^8.632)/g1^26 + (2*t^8.688)/g1^22 + (4*t^8.745)/g1^18 + (2*t^8.802)/g1^14 + t^8.915/g1^6 - (5*t^8.972)/g1^2 - t^4.486/(g1*y) - t^7.287/(g1^15*y) - t^7.457/(g1^3*y) + (g1*t^7.514)/y + (g1^13*t^7.684)/y + t^8.66/(g1^24*y) + t^8.717/(g1^20*y) + (3*t^8.773)/(g1^16*y) + (2*t^8.83)/(g1^12*y) + (3*t^8.887)/(g1^8*y) + (3*t^8.943)/(g1^4*y) - (t^4.486*y)/g1 - (t^7.287*y)/g1^15 - (t^7.457*y)/g1^3 + g1*t^7.514*y + g1^13*t^7.684*y + (t^8.66*y)/g1^24 + (t^8.717*y)/g1^20 + (3*t^8.773*y)/g1^16 + (2*t^8.83*y)/g1^12 + (3*t^8.887*y)/g1^8 + (3*t^8.943*y)/g1^4 |
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 |
---|---|---|---|---|---|---|---|---|---|
54502 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{6}\phi_{1}^{2}$ + ${ }M_{1}M_{2}$ + ${ }M_{3}M_{5}$ | 0.6951 | 0.8532 | 0.8147 | [M:[0.9573, 1.0427, 1.0256, 0.9402, 0.9744, 1.0085], q:[0.5043, 0.5384], qb:[0.453, 0.5214], phi:[0.4957]] | t^2.821 + t^2.872 + t^2.923 + t^2.974 + t^3.026 + t^3.077 + t^3.128 + t^4.205 + t^4.359 + t^4.41 + t^4.462 + t^4.513 + t^4.564 + 2*t^4.615 + t^4.667 + t^4.718 + t^5.641 + t^5.692 + t^5.744 + t^5.795 + 2*t^5.846 + 2*t^5.897 + 2*t^5.949 - t^6. - t^4.487/y - t^4.487*y | detail |