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 |
|---|---|---|---|---|---|---|---|---|---|
| 48162 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}q_{1}^{2}$ + ${ }M_{5}\phi_{1}q_{1}q_{2}$ | 0.6548 | 0.8185 | 0.8 | [M:[1.1429, 0.7143, 0.8571, 0.8095, 0.7619], q:[0.4048, 0.4524], qb:[0.881, 0.7381], phi:[0.381]] | [M:[[12], [18], [-12], [-2], [8]], q:[[-1], [-11]], qb:[[-17], [13]], phi:[[4]]] | {a: 55/84, c: 275/336, M1: 8/7, M2: 5/7, M3: 6/7, M4: 17/21, M5: 16/21, q1: 17/42, q2: 19/42, qb1: 37/42, qb2: 31/42, phi1: 8/21} |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }M_{5}$, ${ }\phi_{1}^{2}$, ${ }M_{4}$, ${ }M_{3}$, ${ }M_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{5}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{4}M_{5}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}M_{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{5}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{5}\phi_{1}q_{1}^{2}$, ${ }\phi_{1}^{3}q_{1}^{2}$ | ${}M_{2}\phi_{1}q_{2}^{2}$ | 0 | t^2.143 + 2*t^2.286 + t^2.429 + t^2.571 + t^3.429 + t^3.571 + t^3.857 + t^4. + t^4.286 + 2*t^4.429 + 4*t^4.571 + 3*t^4.714 + 4*t^4.857 + t^5. + t^5.143 + t^5.571 + 2*t^5.714 + t^5.857 + 2*t^6.143 + 2*t^6.286 + 3*t^6.429 + 3*t^6.571 + 4*t^6.714 + 7*t^6.857 + 6*t^7. + 6*t^7.143 + 2*t^7.286 + 2*t^7.429 + 2*t^7.714 + 3*t^7.857 + 3*t^8. - t^8.286 - t^8.429 + t^8.571 + 5*t^8.714 + 7*t^8.857 - t^4.143/y - t^6.286/y - (2*t^6.429)/y - t^6.571/y + (2*t^7.429)/y + (2*t^7.571)/y + (4*t^7.714)/y + (4*t^7.857)/y + (2*t^8.)/y - t^8.429/y - t^8.571/y - t^8.714/y + t^8.857/y - t^4.143*y - t^6.286*y - 2*t^6.429*y - t^6.571*y + 2*t^7.429*y + 2*t^7.571*y + 4*t^7.714*y + 4*t^7.857*y + 2*t^8.*y - t^8.429*y - t^8.571*y - t^8.714*y + t^8.857*y | g1^18*t^2.143 + 2*g1^8*t^2.286 + t^2.429/g1^2 + t^2.571/g1^12 + g1^12*t^3.429 + g1^2*t^3.571 + t^3.857/g1^18 + t^4./g1^28 + g1^36*t^4.286 + 2*g1^26*t^4.429 + 4*g1^16*t^4.571 + 3*g1^6*t^4.714 + (4*t^4.857)/g1^4 + t^5./g1^14 + t^5.143/g1^24 + g1^30*t^5.571 + 2*g1^20*t^5.714 + g1^10*t^5.857 + (2*t^6.143)/g1^10 + (2*t^6.286)/g1^20 + (2*t^6.429)/g1^30 + g1^54*t^6.429 + t^6.571/g1^40 + 2*g1^44*t^6.571 + 4*g1^34*t^6.714 + 7*g1^24*t^6.857 + 6*g1^14*t^7. + 6*g1^4*t^7.143 + (2*t^7.286)/g1^6 + (2*t^7.429)/g1^16 + t^7.714/g1^36 + g1^48*t^7.714 + t^7.857/g1^46 + 2*g1^38*t^7.857 + t^8./g1^56 + 2*g1^28*t^8. - g1^8*t^8.286 - t^8.429/g1^2 + g1^72*t^8.571 + (3*t^8.714)/g1^22 + 2*g1^62*t^8.714 + (3*t^8.857)/g1^32 + 4*g1^52*t^8.857 - (g1^4*t^4.143)/y - (g1^22*t^6.286)/y - (2*g1^12*t^6.429)/y - (g1^2*t^6.571)/y + (2*g1^26*t^7.429)/y + (2*g1^16*t^7.571)/y + (4*g1^6*t^7.714)/y + (4*t^7.857)/(g1^4*y) + (2*t^8.)/(g1^14*y) - (g1^40*t^8.429)/y - (g1^30*t^8.571)/y - (g1^20*t^8.714)/y + (g1^10*t^8.857)/y - g1^4*t^4.143*y - g1^22*t^6.286*y - 2*g1^12*t^6.429*y - g1^2*t^6.571*y + 2*g1^26*t^7.429*y + 2*g1^16*t^7.571*y + 4*g1^6*t^7.714*y + (4*t^7.857*y)/g1^4 + (2*t^8.*y)/g1^14 - g1^40*t^8.429*y - g1^30*t^8.571*y - g1^20*t^8.714*y + g1^10*t^8.857*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 |
|---|
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 |
|---|
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 |
|---|
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 |
|---|---|---|---|---|---|---|---|---|---|
| 46384 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}\phi_{1}q_{1}^{2}$ | 0.6363 | 0.7853 | 0.8103 | [M:[1.1492, 0.7237, 0.8508, 0.8085], q:[0.4042, 0.4466], qb:[0.872, 0.7449], phi:[0.3831]] | t^2.171 + t^2.298 + t^2.425 + t^2.553 + t^3.447 + t^3.575 + t^3.702 + t^3.829 + t^3.956 + t^4.342 + t^4.47 + 2*t^4.597 + 2*t^4.724 + 3*t^4.851 + t^4.978 + t^5.105 + t^5.619 + t^5.746 + t^5.873 + t^6. - t^4.149/y - t^4.149*y | detail |