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 |
---|---|---|---|---|---|---|---|---|---|
633 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{4}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{5}\phi_{1}\tilde{q}_{2}^{2}$ | 0.6633 | 0.8593 | 0.772 | [M:[1.1588, 1.1588, 0.6825, 0.6825, 0.6825], q:[0.75, 0.4325], qb:[0.4088, 0.4088], phi:[0.5]] | [M:[[1], [1], [-2], [-2], [-2]], q:[[0], [-2]], qb:[[1], [1]], phi:[[0]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}M_{3}$, ${ }M_{4}$, ${ }M_{5}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }M_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{4}M_{5}$, ${ }M_{5}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{3}$, ${ }M_{2}M_{3}$, ${ }M_{1}M_{4}$, ${ }M_{2}M_{4}$, ${ }M_{1}M_{5}$, ${ }M_{2}M_{5}$, ${ }M_{3}q_{1}\tilde{q}_{1}$, ${ }M_{4}q_{1}\tilde{q}_{1}$, ${ }M_{5}q_{1}\tilde{q}_{1}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }M_{5}q_{1}\tilde{q}_{2}$, ${ }M_{3}q_{1}q_{2}$, ${ }M_{4}q_{1}q_{2}$, ${ }M_{5}q_{1}q_{2}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | ${}$ | -4 | 3*t^2.047 + t^2.453 + t^3. + 4*t^3.476 + t^3.547 + 2*t^4.024 + 7*t^4.095 + 3*t^4.5 + t^4.905 + 3*t^5.047 + t^5.453 + 12*t^5.524 + 3*t^5.595 + 2*t^5.929 - 4*t^6. + 4*t^6.071 + 13*t^6.142 + 2*t^6.476 + 6*t^6.547 + 9*t^6.953 + 2*t^7.024 + 7*t^7.095 + t^7.358 - 4*t^7.429 + 3*t^7.5 + 26*t^7.571 + 7*t^7.642 + 2*t^7.976 - 13*t^8.047 + 8*t^8.119 + 22*t^8.19 + 2*t^8.381 - 4*t^8.453 + 4*t^8.524 + 10*t^8.595 - t^4.5/y - (3*t^6.547)/y + (2*t^7.024)/y + (3*t^7.095)/y + (3*t^7.5)/y - (2*t^7.976)/y + (3*t^8.047)/y + (4*t^8.453)/y + (12*t^8.524)/y - (3*t^8.595)/y + (4*t^8.929)/y - t^4.5*y - 3*t^6.547*y + 2*t^7.024*y + 3*t^7.095*y + 3*t^7.5*y - 2*t^7.976*y + 3*t^8.047*y + 4*t^8.453*y + 12*t^8.524*y - 3*t^8.595*y + 4*t^8.929*y | (3*t^2.047)/g1^2 + g1^2*t^2.453 + t^3. + 4*g1*t^3.476 + t^3.547/g1^2 + (2*t^4.024)/g1 + (7*t^4.095)/g1^4 + 3*t^4.5 + g1^4*t^4.905 + (3*t^5.047)/g1^2 + g1^2*t^5.453 + (12*t^5.524)/g1 + (3*t^5.595)/g1^4 + 2*g1^3*t^5.929 - 4*t^6. + (4*t^6.071)/g1^3 + (13*t^6.142)/g1^6 + 2*g1*t^6.476 + (6*t^6.547)/g1^2 + 9*g1^2*t^6.953 + (2*t^7.024)/g1 + (7*t^7.095)/g1^4 + g1^6*t^7.358 - 4*g1^3*t^7.429 + 3*t^7.5 + (26*t^7.571)/g1^3 + (7*t^7.642)/g1^6 + 2*g1*t^7.976 - (13*t^8.047)/g1^2 + (8*t^8.119)/g1^5 + (22*t^8.19)/g1^8 + 2*g1^5*t^8.381 - 4*g1^2*t^8.453 + (4*t^8.524)/g1 + (10*t^8.595)/g1^4 - t^4.5/y - (3*t^6.547)/(g1^2*y) + (2*t^7.024)/(g1*y) + (3*t^7.095)/(g1^4*y) + (3*t^7.5)/y - (2*g1*t^7.976)/y + (3*t^8.047)/(g1^2*y) + (4*g1^2*t^8.453)/y + (12*t^8.524)/(g1*y) - (3*t^8.595)/(g1^4*y) + (4*g1^3*t^8.929)/y - t^4.5*y - (3*t^6.547*y)/g1^2 + (2*t^7.024*y)/g1 + (3*t^7.095*y)/g1^4 + 3*t^7.5*y - 2*g1*t^7.976*y + (3*t^8.047*y)/g1^2 + 4*g1^2*t^8.453*y + (12*t^8.524*y)/g1 - (3*t^8.595*y)/g1^4 + 4*g1^3*t^8.929*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 |
---|---|---|---|---|---|---|---|---|
1955 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{4}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{5}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}q_{1}q_{2}$ | 0.6537 | 0.8412 | 0.7771 | [M:[1.125, 1.125, 0.75, 0.75, 0.75], q:[0.75, 0.5], qb:[0.375, 0.375], phi:[0.5]] | 4*t^2.25 + t^3. + 4*t^3.375 + t^3.75 + 2*t^4.125 + 11*t^4.5 + 4*t^5.25 + 14*t^5.625 - t^6. - t^4.5/y - t^4.5*y | detail | {a: 5355/8192, c: 6891/8192, M1: 9/8, M2: 9/8, M3: 3/4, M4: 3/4, M5: 3/4, q1: 3/4, q2: 1/2, qb1: 3/8, qb2: 3/8, phi1: 1/2} |
1956 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{4}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{5}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{6}q_{1}q_{2}$ | 0.6792 | 0.8856 | 0.7669 | [M:[1.1517, 1.1517, 0.6966, 0.6966, 0.6966, 0.8034], q:[0.75, 0.4466], qb:[0.4017, 0.4017], phi:[0.5]] | 3*t^2.09 + 2*t^2.41 + t^3. + 4*t^3.455 + 2*t^4.045 + 7*t^4.18 + 6*t^4.5 + 3*t^4.82 + 3*t^5.09 + 2*t^5.41 + 12*t^5.545 + 6*t^5.865 - 5*t^6. - t^4.5/y - t^4.5*y | detail |
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 |
---|---|---|---|---|---|---|---|---|---|
392 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{4}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{3}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ | 0.6426 | 0.8185 | 0.785 | [M:[1.1576, 1.1576, 0.6848, 0.6848], q:[0.75, 0.4348], qb:[0.4076, 0.4076], phi:[0.5]] | 2*t^2.054 + t^2.446 + t^3. + 4*t^3.473 + t^3.554 + t^3.946 + 2*t^4.027 + 4*t^4.109 + 2*t^4.5 + t^4.891 + 2*t^5.054 + t^5.446 + 8*t^5.527 + 2*t^5.609 + 2*t^5.919 - 2*t^6. - t^4.5/y - t^4.5*y | detail |