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 |
|---|---|---|---|---|---|---|---|---|---|
| 3635 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}q_{1}q_{2}$ + ${ }M_{1}X_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{1}$ + ${ }M_{5}\phi_{1}\tilde{q}_{1}^{2}$ | 0.6346 | 0.794 | 0.7993 | [X:[1.6], M:[0.4, 1.2, 0.7625, 0.7625, 0.7249], q:[0.8, 0.8], qb:[0.4375, 0.3625], phi:[0.4]] | [X:[[0, 0]], M:[[0, 0], [0, 0], [1, 1], [-1, 1], [0, 2]], q:[[-1, 0], [1, 0]], qb:[[0, -1], [0, 1]], phi:[[0, 0]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{5}$, ${ }M_{4}$, ${ }M_{3}$, ${ }\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{3}M_{5}$, ${ }M_{3}M_{4}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{4}^{2}$, ${ }M_{3}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{4}$, ${ }X_{1}$, ${ }M_{5}\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{5}q_{1}\tilde{q}_{2}$, ${ }M_{4}\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{5}q_{2}\tilde{q}_{2}$, ${ }M_{3}\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }M_{5}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}\tilde{q}_{2}^{2}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{2}M_{4}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }M_{4}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{3}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ | ${}\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}\tilde{q}_{2}$ | -1 | t^2.175 + 2*t^2.287 + t^2.4 + t^3.375 + 2*t^3.487 + 2*t^3.6 + t^4.349 + 2*t^4.462 + 4*t^4.575 + 2*t^4.687 + 2*t^4.8 + t^5.549 + 4*t^5.662 + 6*t^5.775 + 4*t^5.887 - t^6. - 2*t^6.113 - t^6.225 + t^6.524 + 2*t^6.637 + 5*t^6.749 + 8*t^6.862 + 8*t^6.975 + 4*t^7.087 - 4*t^7.313 - 2*t^7.425 + t^7.724 + 4*t^7.837 + 9*t^7.949 + 10*t^8.062 + 5*t^8.175 - 4*t^8.287 - 5*t^8.4 - 6*t^8.513 - 2*t^8.625 + t^8.699 + 2*t^8.811 + 5*t^8.924 - t^4.2/y - t^6.375/y - (2*t^6.487)/y + (2*t^7.462)/y + (2*t^7.575)/y + (2*t^7.687)/y + (2*t^7.913)/y + t^8.025/y + (2*t^8.662)/y + (4*t^8.775)/y + (6*t^8.887)/y - t^4.2*y - t^6.375*y - 2*t^6.487*y + 2*t^7.462*y + 2*t^7.575*y + 2*t^7.687*y + 2*t^7.913*y + t^8.025*y + 2*t^8.662*y + 4*t^8.775*y + 6*t^8.887*y | g2^2*t^2.175 + (g2*t^2.287)/g1 + g1*g2*t^2.287 + t^2.4 + g2^2*t^3.375 + (g2*t^3.487)/g1 + g1*g2*t^3.487 + 2*t^3.6 + g2^4*t^4.349 + (g2^3*t^4.462)/g1 + g1*g2^3*t^4.462 + 2*g2^2*t^4.575 + (g2^2*t^4.575)/g1^2 + g1^2*g2^2*t^4.575 + (g2*t^4.687)/g1 + g1*g2*t^4.687 + 2*t^4.8 + g2^4*t^5.549 + (2*g2^3*t^5.662)/g1 + 2*g1*g2^3*t^5.662 + 4*g2^2*t^5.775 + (g2^2*t^5.775)/g1^2 + g1^2*g2^2*t^5.775 + (2*g2*t^5.887)/g1 + 2*g1*g2*t^5.887 - t^6. - t^6.113/(g1*g2) - (g1*t^6.113)/g2 - t^6.225/g2^2 + g2^6*t^6.524 + (g2^5*t^6.637)/g1 + g1*g2^5*t^6.637 + 3*g2^4*t^6.749 + (g2^4*t^6.749)/g1^2 + g1^2*g2^4*t^6.749 + (g2^3*t^6.862)/g1^3 + (3*g2^3*t^6.862)/g1 + 3*g1*g2^3*t^6.862 + g1^3*g2^3*t^6.862 + 4*g2^2*t^6.975 + (2*g2^2*t^6.975)/g1^2 + 2*g1^2*g2^2*t^6.975 + (2*g2*t^7.087)/g1 + 2*g1*g2*t^7.087 - (2*t^7.313)/(g1*g2) - (2*g1*t^7.313)/g2 - (2*t^7.425)/g2^2 + g2^6*t^7.724 + (2*g2^5*t^7.837)/g1 + 2*g1*g2^5*t^7.837 + 5*g2^4*t^7.949 + (2*g2^4*t^7.949)/g1^2 + 2*g1^2*g2^4*t^7.949 + (g2^3*t^8.062)/g1^3 + (4*g2^3*t^8.062)/g1 + 4*g1*g2^3*t^8.062 + g1^3*g2^3*t^8.062 + g2^2*t^8.175 + (2*g2^2*t^8.175)/g1^2 + 2*g1^2*g2^2*t^8.175 - (2*g2*t^8.287)/g1 - 2*g1*g2*t^8.287 - 3*t^8.4 - t^8.4/g1^2 - g1^2*t^8.4 - (3*t^8.513)/(g1*g2) - (3*g1*t^8.513)/g2 - (2*t^8.625)/g2^2 + g2^8*t^8.699 + (g2^7*t^8.811)/g1 + g1*g2^7*t^8.811 + 3*g2^6*t^8.924 + (g2^6*t^8.924)/g1^2 + g1^2*g2^6*t^8.924 - t^4.2/y - (g2^2*t^6.375)/y - (g2*t^6.487)/(g1*y) - (g1*g2*t^6.487)/y + (g2^3*t^7.462)/(g1*y) + (g1*g2^3*t^7.462)/y + (2*g2^2*t^7.575)/y + (g2*t^7.687)/(g1*y) + (g1*g2*t^7.687)/y + t^7.913/(g1*g2*y) + (g1*t^7.913)/(g2*y) + t^8.025/(g2^2*y) + (g2^3*t^8.662)/(g1*y) + (g1*g2^3*t^8.662)/y + (4*g2^2*t^8.775)/y + (3*g2*t^8.887)/(g1*y) + (3*g1*g2*t^8.887)/y - t^4.2*y - g2^2*t^6.375*y - (g2*t^6.487*y)/g1 - g1*g2*t^6.487*y + (g2^3*t^7.462*y)/g1 + g1*g2^3*t^7.462*y + 2*g2^2*t^7.575*y + (g2*t^7.687*y)/g1 + g1*g2*t^7.687*y + (t^7.913*y)/(g1*g2) + (g1*t^7.913*y)/g2 + (t^8.025*y)/g2^2 + (g2^3*t^8.662*y)/g1 + g1*g2^3*t^8.662*y + 4*g2^2*t^8.775*y + (3*g2*t^8.887*y)/g1 + 3*g1*g2*t^8.887*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 |
|---|---|---|---|---|---|---|---|---|---|
| 3213 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}q_{1}q_{2}$ + ${ }M_{1}X_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{1}$ | 0.615 | 0.7557 | 0.8139 | [X:[1.6], M:[0.4, 1.2, 0.7748, 0.7748], q:[0.8, 0.8], qb:[0.4252, 0.3748], phi:[0.4]] | 2*t^2.324 + t^2.4 + t^3.449 + 2*t^3.524 + 2*t^3.6 + t^3.751 + 3*t^4.649 + 2*t^4.724 + 2*t^4.8 + 2*t^5.773 + 4*t^5.849 + 4*t^5.924 - t^6. - t^4.2/y - t^4.2*y | detail |