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 |
|---|---|---|---|---|---|---|---|---|---|
| 57046 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}\phi_{1}^{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{1}M_{6}$ + ${ }M_{5}^{2}$ + ${ }M_{7}\phi_{1}^{2}$ | 0.6977 | 0.8546 | 0.8164 | [M:[1.0435, 0.9348, 0.9565, 1.0217, 1.0, 0.9565, 1.0217], q:[0.5109, 0.4457], qb:[0.5543, 0.5326], phi:[0.4891]] | [M:[[4], [-6], [-4], [2], [0], [-4], [2]], q:[[1], [-5]], qb:[[5], [3]], phi:[[-1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }M_{3}$, ${ }M_{6}$, ${ }M_{5}$, ${ }M_{4}$, ${ }M_{7}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{6}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{3}M_{5}$, ${ }M_{5}M_{6}$, ${ }M_{2}M_{7}$, ${ }M_{3}M_{4}$, ${ }M_{4}M_{6}$, ${ }M_{3}M_{7}$, ${ }M_{6}M_{7}$ | ${}$ | -3 | t^2.804 + 2*t^2.87 + t^3. + 2*t^3.065 + t^3.261 + t^4.142 + t^4.337 + t^4.402 + t^4.467 + t^4.533 + t^4.598 + 2*t^4.663 + t^4.728 + t^4.793 + t^5.609 + t^5.674 + 2*t^5.739 + 3*t^5.87 + 2*t^5.935 - 3*t^6. + t^6.065 + 3*t^6.13 - t^6.196 + t^6.326 + t^6.521 + t^6.946 + 2*t^7.011 + t^7.142 + 3*t^7.207 + t^7.272 + 2*t^7.337 + 3*t^7.402 + 2*t^7.467 + 3*t^7.533 + 2*t^7.598 + 3*t^7.663 + 2*t^7.728 + t^7.793 + t^7.858 + t^7.924 + t^7.989 + t^8.054 + t^8.283 + t^8.413 + 2*t^8.479 + t^8.544 + 3*t^8.609 + 2*t^8.674 + 2*t^8.739 + t^8.804 - 4*t^8.87 + 3*t^8.935 - t^4.467/y - t^7.272/y - t^7.337/y + t^7.402/y - t^7.533/y + t^7.598/y + t^7.663/y + (2*t^8.674)/y + t^8.739/y + t^8.804/y + (4*t^8.87)/y + (4*t^8.935)/y - t^4.467*y - t^7.272*y - t^7.337*y + t^7.402*y - t^7.533*y + t^7.598*y + t^7.663*y + 2*t^8.674*y + t^8.739*y + t^8.804*y + 4*t^8.87*y + 4*t^8.935*y | t^2.804/g1^6 + (2*t^2.87)/g1^4 + t^3. + 2*g1^2*t^3.065 + g1^8*t^3.261 + t^4.142/g1^11 + t^4.337/g1^5 + t^4.402/g1^3 + t^4.467/g1 + g1*t^4.533 + g1^3*t^4.598 + 2*g1^5*t^4.663 + g1^7*t^4.728 + g1^9*t^4.793 + t^5.609/g1^12 + t^5.674/g1^10 + (2*t^5.739)/g1^8 + (3*t^5.87)/g1^4 + (2*t^5.935)/g1^2 - 3*t^6. + g1^2*t^6.065 + 3*g1^4*t^6.13 - g1^6*t^6.196 + g1^10*t^6.326 + g1^16*t^6.521 + t^6.946/g1^17 + (2*t^7.011)/g1^15 + t^7.142/g1^11 + (3*t^7.207)/g1^9 + t^7.272/g1^7 + (2*t^7.337)/g1^5 + (3*t^7.402)/g1^3 + (2*t^7.467)/g1 + 3*g1*t^7.533 + 2*g1^3*t^7.598 + 3*g1^5*t^7.663 + 2*g1^7*t^7.728 + g1^9*t^7.793 + g1^11*t^7.858 + g1^13*t^7.924 + g1^15*t^7.989 + g1^17*t^8.054 + t^8.283/g1^22 + t^8.413/g1^18 + (2*t^8.479)/g1^16 + t^8.544/g1^14 + (3*t^8.609)/g1^12 + (2*t^8.674)/g1^10 + (2*t^8.739)/g1^8 + t^8.804/g1^6 - (4*t^8.87)/g1^4 + (3*t^8.935)/g1^2 - t^4.467/(g1*y) - t^7.272/(g1^7*y) - t^7.337/(g1^5*y) + t^7.402/(g1^3*y) - (g1*t^7.533)/y + (g1^3*t^7.598)/y + (g1^5*t^7.663)/y + (2*t^8.674)/(g1^10*y) + t^8.739/(g1^8*y) + t^8.804/(g1^6*y) + (4*t^8.87)/(g1^4*y) + (4*t^8.935)/(g1^2*y) - (t^4.467*y)/g1 - (t^7.272*y)/g1^7 - (t^7.337*y)/g1^5 + (t^7.402*y)/g1^3 - g1*t^7.533*y + g1^3*t^7.598*y + g1^5*t^7.663*y + (2*t^8.674*y)/g1^10 + (t^8.739*y)/g1^8 + (t^8.804*y)/g1^6 + (4*t^8.87*y)/g1^4 + (4*t^8.935*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 |
|---|
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 |
|---|---|---|---|---|---|---|---|---|---|
| 55435 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}\phi_{1}^{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{1}M_{6}$ + ${ }M_{5}^{2}$ | 0.6999 | 0.8585 | 0.8152 | [M:[1.0504, 0.9245, 0.9496, 1.0252, 1.0, 0.9496], q:[0.5126, 0.437], qb:[0.563, 0.5378], phi:[0.4874]] | t^2.773 + 2*t^2.849 + t^2.924 + t^3. + t^3.076 + t^3.302 + t^4.085 + t^4.311 + t^4.387 + t^4.462 + t^4.538 + t^4.613 + 2*t^4.689 + t^4.764 + t^4.84 + t^5.547 + t^5.622 + 3*t^5.698 + 2*t^5.773 + 3*t^5.849 + t^5.924 - 2*t^6. - t^4.462/y - t^4.462*y | detail |