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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2282 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}^{2}$ + ${ }M_{4}q_{1}q_{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}\phi_{1}q_{2}^{2}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{7}$ | 0.6987 | 0.8788 | 0.795 | [M:[1.0, 1.1613, 0.9248, 0.8387, 0.7956, 0.7635, 0.8387], q:[0.7796, 0.3818], qb:[0.6182, 0.4569], phi:[0.4409]] | [M:[[0], [-3], [-11], [3], [10], [-8], [3]], q:[[1], [-4]], qb:[[4], [7]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{6}$, ${ }M_{5}$, ${ }M_{4}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{6}^{2}$, ${ }M_{5}M_{6}$, ${ }M_{5}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{6}M_{7}$, ${ }M_{4}M_{5}$, ${ }M_{5}M_{7}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{7}$, ${ }M_{7}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{3}M_{5}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{1}M_{6}$, ${ }M_{3}M_{7}$, ${ }\phi_{1}^{4}$, ${ }M_{1}M_{5}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}M_{7}$, ${ }M_{3}^{2}$, ${ }M_{1}\phi_{1}^{2}$ | ${}$ | -2 | t^2.291 + t^2.387 + 2*t^2.516 + t^2.645 + t^2.774 + t^3. + t^3.839 + t^4.064 + t^4.193 + t^4.323 + t^4.548 + t^4.581 + t^4.677 + t^4.774 + 2*t^4.807 + 2*t^4.903 + t^4.936 + 5*t^5.032 + t^5.065 + 3*t^5.161 + 3*t^5.291 + t^5.387 + t^5.42 + t^5.516 + t^5.549 + t^5.645 - 2*t^6. + 2*t^6.355 + t^6.451 + 3*t^6.58 + t^6.613 + 2*t^6.709 + 3*t^6.839 + t^6.872 + t^6.935 + t^6.968 + 3*t^7.064 + 2*t^7.097 + t^7.161 + 2*t^7.193 + t^7.226 + 2*t^7.29 + 4*t^7.323 + t^7.355 + 4*t^7.419 + 3*t^7.452 + 7*t^7.548 + 3*t^7.581 + 6*t^7.677 + t^7.71 + t^7.774 + 4*t^7.807 + t^7.839 + t^7.903 + 4*t^7.936 + t^8.032 + 2*t^8.065 + t^8.128 + t^8.194 - 2*t^8.291 + t^8.323 - 2*t^8.387 - 6*t^8.516 + t^8.612 - 2*t^8.645 - 3*t^8.774 + t^8.838 + 2*t^8.871 + 3*t^8.967 - t^4.323/y - t^6.613/y - t^6.709/y - t^6.839/y - t^6.968/y - t^7.097/y + t^7.548/y + (2*t^7.677)/y + (3*t^7.807)/y + (2*t^7.903)/y + (2*t^7.936)/y + (3*t^8.032)/y + t^8.065/y + (3*t^8.161)/y + (3*t^8.291)/y + t^8.387/y + t^8.42/y + (2*t^8.516)/y + t^8.645/y + t^8.774/y - t^8.904/y - t^4.323*y - t^6.613*y - t^6.709*y - t^6.839*y - t^6.968*y - t^7.097*y + t^7.548*y + 2*t^7.677*y + 3*t^7.807*y + 2*t^7.903*y + 2*t^7.936*y + 3*t^8.032*y + t^8.065*y + 3*t^8.161*y + 3*t^8.291*y + t^8.387*y + t^8.42*y + 2*t^8.516*y + t^8.645*y + t^8.774*y - t^8.904*y | t^2.291/g1^8 + g1^10*t^2.387 + 2*g1^3*t^2.516 + t^2.645/g1^4 + t^2.774/g1^11 + t^3. + g1*t^3.839 + g1^12*t^4.064 + g1^5*t^4.193 + t^4.323/g1^2 + g1^9*t^4.548 + t^4.581/g1^16 + g1^2*t^4.677 + g1^20*t^4.774 + (2*t^4.807)/g1^5 + 2*g1^13*t^4.903 + t^4.936/g1^12 + 5*g1^6*t^5.032 + t^5.065/g1^19 + (3*t^5.161)/g1 + (3*t^5.291)/g1^8 + g1^10*t^5.387 + t^5.42/g1^15 + g1^3*t^5.516 + t^5.549/g1^22 + t^5.645/g1^4 - 2*t^6. + 2*g1^4*t^6.355 + g1^22*t^6.451 + 3*g1^15*t^6.58 + t^6.613/g1^10 + 2*g1^8*t^6.709 + 3*g1*t^6.839 + t^6.872/g1^24 + g1^19*t^6.935 + t^6.968/g1^6 + 3*g1^12*t^7.064 + (2*t^7.097)/g1^13 + g1^30*t^7.161 + 2*g1^5*t^7.193 + t^7.226/g1^20 + 2*g1^23*t^7.29 + (4*t^7.323)/g1^2 + t^7.355/g1^27 + 4*g1^16*t^7.419 + (3*t^7.452)/g1^9 + 7*g1^9*t^7.548 + (3*t^7.581)/g1^16 + 6*g1^2*t^7.677 + t^7.71/g1^23 + g1^20*t^7.774 + (4*t^7.807)/g1^5 + t^7.839/g1^30 + g1^13*t^7.903 + (4*t^7.936)/g1^12 + g1^6*t^8.032 + (2*t^8.065)/g1^19 + g1^24*t^8.128 + t^8.194/g1^26 - (2*t^8.291)/g1^8 + t^8.323/g1^33 - 2*g1^10*t^8.387 - 6*g1^3*t^8.516 + g1^21*t^8.612 - (2*t^8.645)/g1^4 - (3*t^8.774)/g1^11 + g1^32*t^8.838 + 2*g1^7*t^8.871 + 3*g1^25*t^8.967 - t^4.323/(g1^2*y) - t^6.613/(g1^10*y) - (g1^8*t^6.709)/y - (g1*t^6.839)/y - t^6.968/(g1^6*y) - t^7.097/(g1^13*y) + (g1^9*t^7.548)/y + (2*g1^2*t^7.677)/y + (3*t^7.807)/(g1^5*y) + (2*g1^13*t^7.903)/y + (2*t^7.936)/(g1^12*y) + (3*g1^6*t^8.032)/y + t^8.065/(g1^19*y) + (3*t^8.161)/(g1*y) + (3*t^8.291)/(g1^8*y) + (g1^10*t^8.387)/y + t^8.42/(g1^15*y) + (2*g1^3*t^8.516)/y + t^8.645/(g1^4*y) + t^8.774/(g1^11*y) - t^8.904/(g1^18*y) - (t^4.323*y)/g1^2 - (t^6.613*y)/g1^10 - g1^8*t^6.709*y - g1*t^6.839*y - (t^6.968*y)/g1^6 - (t^7.097*y)/g1^13 + g1^9*t^7.548*y + 2*g1^2*t^7.677*y + (3*t^7.807*y)/g1^5 + 2*g1^13*t^7.903*y + (2*t^7.936*y)/g1^12 + 3*g1^6*t^8.032*y + (t^8.065*y)/g1^19 + (3*t^8.161*y)/g1 + (3*t^8.291*y)/g1^8 + g1^10*t^8.387*y + (t^8.42*y)/g1^15 + 2*g1^3*t^8.516*y + (t^8.645*y)/g1^4 + (t^8.774*y)/g1^11 - (t^8.904*y)/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 |
---|---|---|---|---|---|---|---|---|---|
1229 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}^{2}$ + ${ }M_{4}q_{1}q_{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}\phi_{1}q_{2}^{2}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ | 0.6848 | 0.8548 | 0.8012 | [M:[1.0, 1.1585, 0.9146, 0.8415, 0.8049, 0.7561], q:[0.7805, 0.378], qb:[0.622, 0.4635], phi:[0.439]] | t^2.268 + t^2.415 + t^2.524 + t^2.634 + t^2.744 + t^3. + t^3.476 + t^3.841 + t^4.098 + t^4.207 + t^4.317 + t^4.536 + t^4.573 + t^4.683 + t^4.793 + t^4.83 + t^4.902 + t^4.939 + t^5.012 + 3*t^5.049 + 2*t^5.159 + 2*t^5.268 + t^5.378 + t^5.415 + t^5.487 + t^5.634 + t^5.744 + t^5.89 - t^6. - t^4.317/y - t^4.317*y | detail |