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 |
---|---|---|---|---|---|---|---|---|---|
3233 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{4}$ + ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}q_{1}\tilde{q}_{1}$ | 0.6766 | 0.8814 | 0.7676 | [M:[1.1387, 0.7226, 0.75, 0.8613, 0.75], q:[0.75, 0.3613], qb:[0.5, 0.3887], phi:[0.5]] | [M:[[1], [-2], [0], [-1], [0]], q:[[0], [-1]], qb:[[0], [1]], phi:[[0]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
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${}M_{2}$, ${ }M_{3}$, ${ }M_{5}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{4}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }q_{1}q_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{5}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{5}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{5}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{3}M_{4}$, ${ }M_{4}M_{5}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}q_{1}q_{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{3}q_{1}q_{2}$, ${ }M_{5}q_{1}q_{2}$, ${ }M_{2}q_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}^{2}\tilde{q}_{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }M_{5}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }M_{2}\phi_{1}q_{2}^{2}$, ${ }M_{4}q_{1}q_{2}$, ${ }M_{3}\phi_{1}q_{2}^{2}$, ${ }M_{5}\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{2}$ | ${}M_{4}q_{1}\tilde{q}_{2}$ | -1 | t^2.168 + 3*t^2.25 + t^2.584 + t^2.666 + t^3. + t^3.334 + t^3.416 + t^3.668 + t^4.084 + t^4.166 + t^4.336 + 3*t^4.418 + 7*t^4.5 + t^4.752 + 4*t^4.834 + 3*t^4.916 + 2*t^5.168 + 4*t^5.25 + t^5.332 + t^5.502 + 4*t^5.584 + 3*t^5.666 + t^5.836 + 3*t^5.918 - t^6. + 2*t^6.252 + 3*t^6.334 + t^6.416 + t^6.504 + 3*t^6.586 + 9*t^6.668 + 12*t^6.75 + t^6.832 + t^6.92 + 5*t^7.002 + 8*t^7.084 + 4*t^7.166 + 3*t^7.336 + 6*t^7.418 + 7*t^7.5 + 2*t^7.582 + t^7.67 + 6*t^7.752 + 8*t^7.834 + 4*t^7.916 + t^7.998 + t^8.004 + 3*t^8.086 + 6*t^8.168 - 5*t^8.25 + 2*t^8.42 + 6*t^8.502 + 2*t^8.584 - 2*t^8.666 + t^8.672 + 3*t^8.754 + 10*t^8.836 + 15*t^8.918 - t^4.5/y - t^6.668/y - (2*t^6.75)/y + (3*t^7.418)/y + (3*t^7.5)/y + t^7.752/y + (4*t^7.834)/y + (3*t^7.916)/y + t^8.168/y + (6*t^8.25)/y + t^8.332/y + t^8.502/y + (5*t^8.584)/y + (4*t^8.666)/y + (2*t^8.918)/y - t^4.5*y - t^6.668*y - 2*t^6.75*y + 3*t^7.418*y + 3*t^7.5*y + t^7.752*y + 4*t^7.834*y + 3*t^7.916*y + t^8.168*y + 6*t^8.25*y + t^8.332*y + t^8.502*y + 5*t^8.584*y + 4*t^8.666*y + 2*t^8.918*y | t^2.168/g1^2 + 3*t^2.25 + t^2.584/g1 + g1*t^2.666 + t^3. + t^3.334/g1 + g1*t^3.416 + t^3.668/g1^2 + t^4.084/g1 + g1*t^4.166 + t^4.336/g1^4 + (3*t^4.418)/g1^2 + 7*t^4.5 + t^4.752/g1^3 + (4*t^4.834)/g1 + 3*g1*t^4.916 + (2*t^5.168)/g1^2 + 4*t^5.25 + g1^2*t^5.332 + t^5.502/g1^3 + (4*t^5.584)/g1 + 3*g1*t^5.666 + t^5.836/g1^4 + (3*t^5.918)/g1^2 - t^6. + (2*t^6.252)/g1^3 + (3*t^6.334)/g1 + g1*t^6.416 + t^6.504/g1^6 + (3*t^6.586)/g1^4 + (9*t^6.668)/g1^2 + 12*t^6.75 + g1^2*t^6.832 + t^6.92/g1^5 + (5*t^7.002)/g1^3 + (8*t^7.084)/g1 + 4*g1*t^7.166 + (3*t^7.336)/g1^4 + (6*t^7.418)/g1^2 + 7*t^7.5 + 2*g1^2*t^7.582 + t^7.67/g1^5 + (6*t^7.752)/g1^3 + (8*t^7.834)/g1 + 4*g1*t^7.916 + g1^3*t^7.998 + t^8.004/g1^6 + (3*t^8.086)/g1^4 + (6*t^8.168)/g1^2 - 5*t^8.25 + (2*t^8.42)/g1^5 + (6*t^8.502)/g1^3 + (2*t^8.584)/g1 - 2*g1*t^8.666 + t^8.672/g1^8 + (3*t^8.754)/g1^6 + (10*t^8.836)/g1^4 + (15*t^8.918)/g1^2 - t^4.5/y - t^6.668/(g1^2*y) - (2*t^6.75)/y + (3*t^7.418)/(g1^2*y) + (3*t^7.5)/y + t^7.752/(g1^3*y) + (4*t^7.834)/(g1*y) + (3*g1*t^7.916)/y + t^8.168/(g1^2*y) + (6*t^8.25)/y + (g1^2*t^8.332)/y + t^8.502/(g1^3*y) + (5*t^8.584)/(g1*y) + (4*g1*t^8.666)/y + (2*t^8.918)/(g1^2*y) - t^4.5*y - (t^6.668*y)/g1^2 - 2*t^6.75*y + (3*t^7.418*y)/g1^2 + 3*t^7.5*y + (t^7.752*y)/g1^3 + (4*t^7.834*y)/g1 + 3*g1*t^7.916*y + (t^8.168*y)/g1^2 + 6*t^8.25*y + g1^2*t^8.332*y + (t^8.502*y)/g1^3 + (5*t^8.584*y)/g1 + 4*g1*t^8.666*y + (2*t^8.918*y)/g1^2 |
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 |
---|---|---|---|---|---|---|---|---|
3653 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{4}$ + ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}q_{1}\tilde{q}_{1}$ + ${ }M_{2}q_{1}q_{2}$ | 0.6676 | 0.8656 | 0.7713 | [M:[1.0833, 0.8333, 0.75, 0.9167, 0.75], q:[0.75, 0.4167], qb:[0.5, 0.3333], phi:[0.5]] | 3*t^2.25 + 2*t^2.5 + t^2.75 + t^3. + t^3.25 + t^3.5 + 2*t^4. + t^4.25 + 7*t^4.5 + 6*t^4.75 + 6*t^5. + 5*t^5.25 + 5*t^5.5 + 4*t^5.75 - t^4.5/y - t^4.5*y | detail | {a: 2051/3072, c: 2659/3072, M1: 13/12, M2: 5/6, M3: 3/4, M4: 11/12, M5: 3/4, q1: 3/4, q2: 5/12, qb1: 1/2, qb2: 1/3, phi1: 1/2} |
3654 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{4}$ + ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}q_{1}\tilde{q}_{1}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ | 0.6893 | 0.9051 | 0.7616 | [M:[1.1508, 0.6985, 0.75, 0.8492, 0.75, 0.8492], q:[0.75, 0.3492], qb:[0.5, 0.4008], phi:[0.5]] | t^2.095 + 3*t^2.25 + 2*t^2.548 + t^2.702 + t^3. + t^3.298 + t^3.595 + t^4.048 + t^4.191 + t^4.202 + 3*t^4.345 + 7*t^4.5 + 2*t^4.643 + 7*t^4.798 + 3*t^4.952 + 4*t^5.095 + 5*t^5.25 + t^5.393 + t^5.405 + 4*t^5.548 + t^5.691 + 4*t^5.845 - 2*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 |
---|---|---|---|---|---|---|---|---|---|
2719 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }\phi_{1}^{4}$ + ${ }M_{2}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{1}M_{4}$ | 0.6575 | 0.8468 | 0.7765 | [M:[1.1387, 0.7226, 0.75, 0.8613], q:[0.75, 0.3613], qb:[0.5, 0.3887], phi:[0.5]] | t^2.168 + 2*t^2.25 + t^2.584 + t^2.666 + t^3. + t^3.334 + t^3.416 + t^3.668 + t^3.75 + t^4.084 + t^4.166 + t^4.336 + 2*t^4.418 + 4*t^4.5 + t^4.752 + 3*t^4.834 + 2*t^4.916 + 2*t^5.168 + 3*t^5.25 + t^5.332 + t^5.502 + 3*t^5.584 + 2*t^5.666 + t^5.836 + 3*t^5.918 + t^6. - t^4.5/y - t^4.5*y | detail |