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 |
|---|---|---|---|---|---|---|---|---|---|
| 6044 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}M_{3}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{4}M_{6}$ + ${ }M_{1}M_{7}$ + ${ }M_{8}q_{1}\tilde{q}_{2}$ + ${ }M_{3}M_{9}$ | 0.6944 | 0.8519 | 0.8151 | [M:[1.008, 0.976, 1.024, 0.9601, 1.0399, 1.0399, 0.992, 0.9441, 0.976], q:[0.504, 0.488], qb:[0.4721, 0.5519], phi:[0.496]] | [M:[[2], [-6], [6], [-10], [10], [10], [-2], [-14], [-6]], q:[[1], [-3]], qb:[[-7], [13]], phi:[[-1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{8}$, ${ }M_{2}$, ${ }M_{9}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{5}$, ${ }M_{6}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{8}^{2}$, ${ }M_{2}M_{8}$, ${ }M_{8}M_{9}$, ${ }M_{7}M_{8}$, ${ }M_{8}\phi_{1}^{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{9}$, ${ }M_{9}^{2}$, ${ }M_{2}M_{7}$, ${ }M_{7}M_{9}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{9}\phi_{1}^{2}$, ${ }M_{7}^{2}$, ${ }M_{5}M_{8}$, ${ }M_{6}M_{8}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$ | ${}$ | -4 | t^2.832 + 2*t^2.928 + 2*t^2.976 + 2*t^3.12 + t^4.32 + t^4.368 + 2*t^4.416 + t^4.464 + t^4.512 + t^4.56 + t^4.608 + t^4.656 + t^4.799 + t^5.665 + t^5.76 + t^5.808 + 2*t^5.856 + 3*t^5.904 + 3*t^5.952 - 4*t^6. + t^6.048 + 3*t^6.096 - t^6.144 - t^6.192 + 2*t^6.24 + t^7.153 + t^7.201 + 3*t^7.248 + 3*t^7.296 + 4*t^7.344 + 4*t^7.392 + 2*t^7.44 + t^7.488 + 2*t^7.536 + 2*t^7.584 + 2*t^7.632 - t^7.68 + 2*t^7.728 + 3*t^7.775 - t^7.823 + 2*t^7.919 + t^8.497 + t^8.593 + 2*t^8.641 + 2*t^8.689 + 2*t^8.736 + 5*t^8.784 + 2*t^8.832 + 4*t^8.88 - 2*t^8.928 - 6*t^8.976 - t^4.488/y - t^7.32/y + t^7.368/y - t^7.416/y - t^7.464/y + t^7.512/y + t^7.56/y - t^7.608/y + t^7.656/y + (2*t^8.76)/y + (2*t^8.808)/y + t^8.856/y + (4*t^8.904)/y + (3*t^8.952)/y - t^4.488*y - t^7.32*y + t^7.368*y - t^7.416*y - t^7.464*y + t^7.512*y + t^7.56*y - t^7.608*y + t^7.656*y + 2*t^8.76*y + 2*t^8.808*y + t^8.856*y + 4*t^8.904*y + 3*t^8.952*y | t^2.832/g1^14 + (2*t^2.928)/g1^6 + (2*t^2.976)/g1^2 + 2*g1^10*t^3.12 + t^4.32/g1^15 + t^4.368/g1^11 + (2*t^4.416)/g1^7 + t^4.464/g1^3 + g1*t^4.512 + g1^5*t^4.56 + g1^9*t^4.608 + g1^13*t^4.656 + g1^25*t^4.799 + t^5.665/g1^28 + t^5.76/g1^20 + t^5.808/g1^16 + (2*t^5.856)/g1^12 + (3*t^5.904)/g1^8 + (3*t^5.952)/g1^4 - 4*t^6. + g1^4*t^6.048 + 3*g1^8*t^6.096 - g1^12*t^6.144 - g1^16*t^6.192 + 2*g1^20*t^6.24 + t^7.153/g1^29 + t^7.201/g1^25 + (3*t^7.248)/g1^21 + (3*t^7.296)/g1^17 + (4*t^7.344)/g1^13 + (4*t^7.392)/g1^9 + (2*t^7.44)/g1^5 + t^7.488/g1 + 2*g1^3*t^7.536 + 2*g1^7*t^7.584 + 2*g1^11*t^7.632 - g1^15*t^7.68 + 2*g1^19*t^7.728 + 3*g1^23*t^7.775 - g1^27*t^7.823 + 2*g1^35*t^7.919 + t^8.497/g1^42 + t^8.593/g1^34 + (2*t^8.641)/g1^30 + (2*t^8.689)/g1^26 + (2*t^8.736)/g1^22 + (5*t^8.784)/g1^18 + (2*t^8.832)/g1^14 + (4*t^8.88)/g1^10 - (2*t^8.928)/g1^6 - (6*t^8.976)/g1^2 - t^4.488/(g1*y) - t^7.32/(g1^15*y) + t^7.368/(g1^11*y) - t^7.416/(g1^7*y) - t^7.464/(g1^3*y) + (g1*t^7.512)/y + (g1^5*t^7.56)/y - (g1^9*t^7.608)/y + (g1^13*t^7.656)/y + (2*t^8.76)/(g1^20*y) + (2*t^8.808)/(g1^16*y) + t^8.856/(g1^12*y) + (4*t^8.904)/(g1^8*y) + (3*t^8.952)/(g1^4*y) - (t^4.488*y)/g1 - (t^7.32*y)/g1^15 + (t^7.368*y)/g1^11 - (t^7.416*y)/g1^7 - (t^7.464*y)/g1^3 + g1*t^7.512*y + g1^5*t^7.56*y - g1^9*t^7.608*y + g1^13*t^7.656*y + (2*t^8.76*y)/g1^20 + (2*t^8.808*y)/g1^16 + (t^8.856*y)/g1^12 + (4*t^8.904*y)/g1^8 + (3*t^8.952*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 |
|---|
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 |
|---|---|---|---|---|---|---|---|---|---|
| 4550 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}M_{3}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{4}M_{6}$ + ${ }M_{1}M_{7}$ + ${ }M_{8}q_{1}\tilde{q}_{2}$ | 0.6926 | 0.8487 | 0.8161 | [M:[1.005, 0.985, 1.015, 0.9749, 1.0251, 1.0251, 0.995, 0.9649], q:[0.5025, 0.4925], qb:[0.4824, 0.5326], phi:[0.4975]] | t^2.895 + t^2.955 + 2*t^2.985 + t^3.045 + 2*t^3.075 + t^4.387 + t^4.417 + 2*t^4.447 + t^4.477 + t^4.508 + t^4.538 + t^4.568 + t^4.598 + t^4.688 + t^5.789 + t^5.88 + 2*t^5.94 + 3*t^5.97 - 3*t^6. - t^4.492/y - t^4.492*y | detail |