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 |
|---|---|---|---|---|---|---|---|---|---|
| 52443 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{3}M_{4}$ + ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}M_{5}$ + ${ }M_{2}M_{6}$ | 0.6915 | 0.8487 | 0.8148 | [M:[0.9977, 1.0113, 1.0068, 0.9932, 0.9932, 0.9887], q:[0.4966, 0.5057], qb:[0.4921, 0.5011], phi:[0.5011]] | [M:[[-2], [10], [6], [-6], [-6], [-10]], q:[[-3], [5]], qb:[[-7], [1]], phi:[[1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{6}$, ${ }M_{4}$, ${ }M_{5}$, ${ }M_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{6}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{6}q_{2}\tilde{q}_{1}$, ${ }M_{6}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}M_{5}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }M_{5}q_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$ | ${}\phi_{1}^{2}q_{1}\tilde{q}_{2}$ | -1 | t^2.966 + 2*t^2.98 + 3*t^2.993 + t^3.007 + t^4.456 + t^4.469 + 2*t^4.483 + 2*t^4.497 + 2*t^4.51 + t^4.524 + t^4.537 + t^5.932 + 2*t^5.946 + 5*t^5.959 + 5*t^5.973 + 4*t^5.986 - t^6. - 2*t^6.014 - 2*t^6.027 - t^6.041 + t^7.422 + 3*t^7.435 + 5*t^7.449 + 6*t^7.463 + 6*t^7.476 + 5*t^7.49 + 3*t^7.503 + t^7.517 + t^8.898 + 3*t^8.912 + 6*t^8.925 + 9*t^8.939 + 10*t^8.952 + 5*t^8.966 - t^8.98 - 7*t^8.993 - t^4.503/y - t^7.483/y + t^7.524/y + (2*t^8.946)/y + (4*t^8.959)/y + (7*t^8.973)/y + (5*t^8.986)/y - t^4.503*y - t^7.483*y + t^7.524*y + 2*t^8.946*y + 4*t^8.959*y + 7*t^8.973*y + 5*t^8.986*y | t^2.966/g1^10 + (2*t^2.98)/g1^6 + (3*t^2.993)/g1^2 + g1^2*t^3.007 + t^4.456/g1^13 + t^4.469/g1^9 + (2*t^4.483)/g1^5 + (2*t^4.497)/g1 + 2*g1^3*t^4.51 + g1^7*t^4.524 + g1^11*t^4.537 + t^5.932/g1^20 + (2*t^5.946)/g1^16 + (5*t^5.959)/g1^12 + (5*t^5.973)/g1^8 + (4*t^5.986)/g1^4 - t^6. - 2*g1^4*t^6.014 - 2*g1^8*t^6.027 - g1^12*t^6.041 + t^7.422/g1^23 + (3*t^7.435)/g1^19 + (5*t^7.449)/g1^15 + (6*t^7.463)/g1^11 + (6*t^7.476)/g1^7 + (5*t^7.49)/g1^3 + 3*g1*t^7.503 + g1^5*t^7.517 + t^8.898/g1^30 + (3*t^8.912)/g1^26 + (6*t^8.925)/g1^22 + (9*t^8.939)/g1^18 + (10*t^8.952)/g1^14 + (5*t^8.966)/g1^10 - t^8.98/g1^6 - (7*t^8.993)/g1^2 - (g1*t^4.503)/y - t^7.483/(g1^5*y) + (g1^7*t^7.524)/y + (2*t^8.946)/(g1^16*y) + (4*t^8.959)/(g1^12*y) + (7*t^8.973)/(g1^8*y) + (5*t^8.986)/(g1^4*y) - g1*t^4.503*y - (t^7.483*y)/g1^5 + g1^7*t^7.524*y + (2*t^8.946*y)/g1^16 + (4*t^8.959*y)/g1^12 + (7*t^8.973*y)/g1^8 + (5*t^8.986*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 |
|---|---|---|---|---|---|---|---|---|
| 56352 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{3}M_{4}$ + ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}M_{5}$ + ${ }M_{2}M_{6}$ + ${ }M_{7}\phi_{1}^{2}$ | 0.6918 | 0.8503 | 0.8136 | [M:[0.9952, 1.0241, 1.0145, 0.9855, 0.9855, 0.9759, 0.9952], q:[0.4928, 0.5121], qb:[0.4831, 0.5024], phi:[0.5024]] | t^2.928 + 2*t^2.957 + 4*t^2.986 + t^4.406 + t^4.435 + 2*t^4.464 + 2*t^4.493 + 2*t^4.522 + t^4.551 + t^4.58 + t^5.855 + 2*t^5.884 + 6*t^5.913 + 6*t^5.942 + 6*t^5.971 - 4*t^6. - t^4.507/y - t^4.507*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 |
|---|
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 |
|---|---|---|---|---|---|---|---|---|---|
| 47086 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{3}M_{4}$ + ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}M_{5}$ | 0.6935 | 0.8487 | 0.8171 | [M:[1.0106, 0.9469, 0.9681, 1.0319, 1.0319], q:[0.5159, 0.4734], qb:[0.5372, 0.4947], phi:[0.4947]] | t^2.841 + t^2.968 + 3*t^3.032 + 2*t^3.096 + t^4.325 + t^4.388 + 2*t^4.452 + 2*t^4.516 + 2*t^4.58 + t^4.643 + t^4.707 + t^5.681 + t^5.872 - t^6. - t^4.484/y - t^4.484*y | detail |