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 |
|---|---|---|---|---|---|---|---|---|---|
| 57696 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{5}^{2}$ + ${ }M_{1}M_{6}$ + ${ }M_{2}M_{3}$ + ${ }M_{3}M_{7}$ | 0.6948 | 0.8506 | 0.8168 | [M:[1.0285, 1.0285, 0.9715, 0.943, 1.0, 0.9715, 1.0285], q:[0.4715, 0.5], qb:[0.5, 0.557], phi:[0.4929]] | [M:[[4], [4], [-4], [-8], [0], [-4], [4]], q:[[-4], [0]], qb:[[0], [8]], phi:[[-1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{4}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{5}$, ${ }M_{2}$, ${ }M_{7}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{5}M_{6}$, ${ }M_{4}M_{7}$, ${ }\phi_{1}^{4}$, ${ }M_{5}\phi_{1}^{2}$ | ${}M_{2}M_{6}$, ${ }M_{6}M_{7}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$ | -2 | t^2.829 + t^2.914 + t^2.957 + t^3. + 2*t^3.086 + t^3.171 + t^4.308 + 2*t^4.393 + 3*t^4.479 + t^4.564 + 2*t^4.65 + t^4.821 + t^5.658 + t^5.786 + t^5.872 + 2*t^5.914 + t^5.957 - 2*t^6. + 2*t^6.043 + t^6.128 + 2*t^6.171 + t^6.257 + t^6.342 + t^7.137 + 2*t^7.222 + t^7.265 + 3*t^7.308 + t^7.35 + 4*t^7.393 + t^7.436 + 4*t^7.479 - 2*t^7.521 + 4*t^7.564 + t^7.607 + 4*t^7.65 - 2*t^7.692 + 3*t^7.735 + t^7.778 + 2*t^7.821 - t^7.863 + 2*t^7.906 + t^7.992 + t^8.487 + 2*t^8.615 + 2*t^8.701 + t^8.743 + 3*t^8.786 - 4*t^8.829 + 7*t^8.872 - 6*t^8.914 + 5*t^8.957 - t^4.479/y - t^7.308/y + t^7.393/y - t^7.436/y + t^7.521/y - t^7.564/y + t^7.65/y + t^8.743/y + t^8.786/y + t^8.829/y + t^8.872/y + (3*t^8.914)/y + t^8.957/y - t^4.479*y - t^7.308*y + t^7.393*y - t^7.436*y + t^7.521*y - t^7.564*y + t^7.65*y + t^8.743*y + t^8.786*y + t^8.829*y + t^8.872*y + 3*t^8.914*y + t^8.957*y | t^2.829/g1^8 + t^2.914/g1^4 + t^2.957/g1^2 + t^3. + 2*g1^4*t^3.086 + g1^8*t^3.171 + t^4.308/g1^9 + (2*t^4.393)/g1^5 + (3*t^4.479)/g1 + g1^3*t^4.564 + 2*g1^7*t^4.65 + g1^15*t^4.821 + t^5.658/g1^16 + t^5.786/g1^10 + t^5.872/g1^6 + (2*t^5.914)/g1^4 + t^5.957/g1^2 - 2*t^6. + 2*g1^2*t^6.043 + g1^6*t^6.128 + 2*g1^8*t^6.171 + g1^12*t^6.257 + g1^16*t^6.342 + t^7.137/g1^17 + (2*t^7.222)/g1^13 + t^7.265/g1^11 + (3*t^7.308)/g1^9 + t^7.35/g1^7 + (4*t^7.393)/g1^5 + t^7.436/g1^3 + (4*t^7.479)/g1 - 2*g1*t^7.521 + 4*g1^3*t^7.564 + g1^5*t^7.607 + 4*g1^7*t^7.65 - 2*g1^9*t^7.692 + 3*g1^11*t^7.735 + g1^13*t^7.778 + 2*g1^15*t^7.821 - g1^17*t^7.863 + 2*g1^19*t^7.906 + g1^23*t^7.992 + t^8.487/g1^24 + (2*t^8.615)/g1^18 + (2*t^8.701)/g1^14 + t^8.743/g1^12 + (3*t^8.786)/g1^10 - (4*t^8.829)/g1^8 + (7*t^8.872)/g1^6 - (6*t^8.914)/g1^4 + (5*t^8.957)/g1^2 - t^4.479/(g1*y) - t^7.308/(g1^9*y) + t^7.393/(g1^5*y) - t^7.436/(g1^3*y) + (g1*t^7.521)/y - (g1^3*t^7.564)/y + (g1^7*t^7.65)/y + t^8.743/(g1^12*y) + t^8.786/(g1^10*y) + t^8.829/(g1^8*y) + t^8.872/(g1^6*y) + (3*t^8.914)/(g1^4*y) + t^8.957/(g1^2*y) - (t^4.479*y)/g1 - (t^7.308*y)/g1^9 + (t^7.393*y)/g1^5 - (t^7.436*y)/g1^3 + g1*t^7.521*y - g1^3*t^7.564*y + g1^7*t^7.65*y + (t^8.743*y)/g1^12 + (t^8.786*y)/g1^10 + (t^8.829*y)/g1^8 + (t^8.872*y)/g1^6 + (3*t^8.914*y)/g1^4 + (t^8.957*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 |
|---|---|---|---|---|---|---|---|---|---|
| 55955 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{5}^{2}$ + ${ }M_{1}M_{6}$ + ${ }M_{2}M_{3}$ | 0.698 | 0.8561 | 0.8153 | [M:[1.0398, 1.0398, 0.9602, 0.9204, 1.0, 0.9602], q:[0.4602, 0.5], qb:[0.5, 0.5796], phi:[0.4901]] | t^2.761 + 2*t^2.881 + t^2.94 + t^3. + t^3.119 + t^3.239 + t^4.231 + 2*t^4.351 + 3*t^4.47 + t^4.59 + 2*t^4.709 + t^4.948 + t^5.523 + t^5.642 + t^5.702 + 2*t^5.761 + 2*t^5.821 + 2*t^5.881 + t^5.94 - 2*t^6. - t^4.47/y - t^4.47*y | detail |